Article Superstructures and magnetic order in heavily Cu-substituted (Fe1−𝑥⁢Cu𝑥)1+𝑦⁢Te

Saizheng Cao ORCID ; Xin Ma ; Dongsheng Yuan SAMURAI ORCID ; Zhen Tao ; Xiang Chen ; Yu He ; Patrick N. Valdivia ; Shan Wu ORCID ; Hang Su ; Wei Tian ; Adam A. Aczel ORCID ; Yaohua Liu ORCID ; Xiaoping Wang ORCID ; Zhijun Xu ; Huiqiu Yuan ; Edith Bourret-Courchesne ORCID ; Chao Cao ; Xingye Lu ; Robert Birgeneau ; Yu Song ORCID

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Saizheng Cao, Xin Ma, Dongsheng Yuan, Zhen Tao, Xiang Chen, Yu He, Patrick N. Valdivia, Shan Wu, Hang Su, Wei Tian, Adam A. Aczel, Yaohua Liu, Xiaoping Wang, Zhijun Xu, Huiqiu Yuan, Edith Bourret-Courchesne, Chao Cao, Xingye Lu, Robert Birgeneau, Yu Song. Superstructures and magnetic order in heavily Cu-substituted (Fe1−𝑥⁢Cu𝑥)1+𝑦⁢Te. PHYSICAL REVIEW B. 2024, 109 (4), 045142. https://doi.org/10.1103/physrevb.109.045142
SAMURAI

Description:

(abstract)

Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = . In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1−xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = . Here, we use elastic neutron scattering to investigate heavily Cu-substituted (Fe1−xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range magnetic order emerges around the stripe-type vector at Q = (x) with δ ≈ 0.05; (2)the short-range magnetic order is associated with a superstructure modulation at Q = , with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = and magnetic peaks at Q = . The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by √2× 3√2 times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings.

Description:

(abstract)

Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = . In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1−xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = . Here, we use elastic neutron scattering to
investigate heavily Cu-substituted (Fe1−xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range
magnetic order emerges around the stripe-type vector at Q = (x) with δ ≈ 0.05; (2)the short-range magnetic order is associated with a superstructure modulation at Q = , with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = and magnetic peaks at Q = . The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by √2× 3√2 times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings.

Description:

(abstract)

Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = . In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1−xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = . Here, we use elastic neutron scattering to
investigate heavily Cu-substituted (Fe1−xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range
magnetic order emerges around the stripe-type vector at Q = (x) with δ ≈ 0.05; (2)the short-range magnetic order is associated with a superstructure modulation at Q = , with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = and magnetic peaks at Q = . The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by √2× 3√2 times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings.

Description:

(abstract)

Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = . In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1−xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = . Here, we use elastic neutron scattering to
investigate heavily Cu-substituted (Fe1−xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range
magnetic order emerges around the stripe-type vector at Q = (x) with δ ≈ 0.05; (2)the short-range magnetic order is associated with a superstructure modulation at Q = , with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = and magnetic peaks at Q = . The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by √2× 3√2 times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings.

Description:

(abstract)

Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = . In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1−xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = . Here, we use elastic neutron scattering to
investigate heavily Cu-substituted (Fe1−xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range
magnetic order emerges around the stripe-type vector at Q = (x) with δ ≈ 0.05; (2)the short-range magnetic order is associated with a superstructure modulation at Q = , with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = and magnetic peaks at Q = . The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by √2× 3√2 times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings.

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Keyword: Magnetic order, Structural properties, Iron-based superconductors, Neutron scattering

Date published: 2024-01-23

Publisher:

Journal:

  • PHYSICAL REVIEW B (ISSN: 24699950) vol. 109 issue. 4 045142

Funding:

  • Zhejiang University
  • National Key Research and Development Program of China 2022YFA1402200
  • National Key Research and Development Program of China 2021C01002
  • Beijing Normal University
  • National Natural Science Foundation of China 12274363
  • National Natural Science Foundation of China 12274364
  • National Natural Science Foundation of China 12174029
  • University of California
  • Lawrence Berkeley National Laboratory
  • Office of Science
  • Basic Energy Sciences
  • U.S. Department of Energy DE-AC02-05-CH11231
  • Oak Ridge National Laboratory

Manuscript type: Author's version (Submitted manuscript)

MDR DOI: https://doi.org/10.48505/nims.4991

First published URL: https://doi.org/10.1103/physrevb.109.045142

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Updated at: 2024-12-24 12:09:02 +0900

Published on MDR: 2024-11-19 16:30:51 +0900

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