Journal article Ferrimagnetic structures with rare-earth induced spin-reorientation in the Mn self-doped perovskite (Er0.7Mn0.3)MnO3
Andreas Dönni (author) (Search by this author)
ORCID SAMURAI ;
Vladimir Y. Pomjakushin (author) (Search by this author)
;
Martin Rotter (author) (Search by this author)
;
Lei Zhang (author) (Search by this author)
ORCID https://orcid.org/0000-0003-1173-4328 (unauthenticated)
National Institute for Materials Science
ORCID ;
Kazunari Yamaura (author) (Search by this author)
ORCID SAMURAI ;
Alexei A. Belik (author) (Search by this author)
ORCID SAMURAI
Collection

Citation
Andreas Dönni, Vladimir Y. Pomjakushin, Martin Rotter, Lei Zhang, Kazunari Yamaura, Alexei A. Belik. Ferrimagnetic structures with rare-earth induced spin-reorientation in the Mn self-doped perovskite (Er0.7Mn0.3)MnO3. Ceramics International. 2024, 50 (21), 43414-43423. https://doi.org/10.1016/j.ceramint.2024.08.191

Description:

(abstract)

The search for spin-reorientation (SR) phase transitions, a spontaneous rotation of ordered magnetic moments, in ferrimagnetic (FiM) materials, which carry a net magnetization, is of fundamental and practical interest for applications in the field of spintronics. In this work, we have investigated Mn self-doped (Er0.7Mn0.3)MnO3 solid solution with GdFeO3-type Pnma perovskite structure by combining specific heat, magnetic susceptibility and neutron powder diffraction measurements. We provide experimental evidence for FiM order below TC = 104 K, and a spontaneous SR transition at TSR = 11 K. A FiM structure appears in all (R1-xMnx)MnO3 compounds with R = Dy-Lu for x >= 0.2. But in this structural family, R = Er is the only material with a SR transition. FiM order in (Er0.7Mn0.3)MnO3 appears with ferromagnetic (FM) ordering of Mn3+ and Mn4+ cations at the B site along the a-direction, which are antiferromagnetically (AFM) coupled with Er3+ and Mn2+ cations at the A site. At TSR, ordered Er3+ change direction from the magnetically harder a-axis to the magnetically easy b-axis and induce a change of the whole FiM structure, including the direction of all Mn spins from the irreducible representation mGM3+ to mGM4+. We calculated the crystal-field (CF) anisotropy for Ho3+ in (Ho0.8Mn0.2)MnO3 and Er3+ in (Er0.7Mn0.3)MnO3, based on the point charge model, and showed large magnetic anisotropies. For the FiM structure of (Ho0.8Mn0.2)MnO3, the magnetically easy a-axis of Ho3+ keeps the high-temperature magnetic directions along the a-axis and gives rise to a pronounced magnetization reversal effect at low temperature because of a significant rise of Ho3+ ordered moments. On the other hand, for the FiM structure of (Er0.7Mn0.3)MnO3, the magnetically easy b-axis of Er3+ gives rise to a SR phase transition at TSR, which does not lead to magnetization reversal even though Er3+ ordered moments rise significantly at low temperatures.

Rights:

Keyword: Perovskites, Crystal structure, magnetic structure, spin-reorientation, ferrimagnets

Date published: 2024-08-12

Publisher: Elsevier BV

Journal:

  • Ceramics International (ISSN: 02728842) vol. 50 issue. 21 p. 43414-43423

Funding:

  • World Cancer Research Fund International
  • Japan Society for the Promotion of Science JP22H04601
  • The Kazuchika Okura Memorial Foundation 2022-11

Manuscript type: Author's version (Accepted manuscript)

MDR DOI: https://doi.org/10.48505/nims.4788

First published URL: https://doi.org/10.1016/j.ceramint.2024.08.191

Related item:

Other identifier(s):

Contact agent:

Updated at: 2024-10-02 10:15:50 +0900

Published on MDR: 2026-08-12 08:30:01 +0900

Filename Size
Filename Ceramics International-V50-43414-ErMnO3-Mn_Accepted_Version.pdf
application/pdf
Size 1.54 MB Detail
Filename Ceramics International-V50-43414_Supplement.pdf (Thumbnail)
application/pdf
Size 554 KB Detail