Intrinsic magnetic properties and domain structure of ThMn12-type (Sm, Zr)(Fe, Co, M)12 (M <b>=</b> Ti, Mo) compounds

S Shaohua Fan (School of Materials Science and Engineering of Shanxi Normal University & Key Laboratory of Magnetic Molecules and Magnetic Information Materials of Ministry of Education) Z Zhongchong Lin (Fujian Provincial Key Laboratory of Quantum Manipulation and New Energy Materials, College of Physics and Energy) B Baochun Wu (State Key Laboratory of Low Dimensional Quantum Physics and Department of Physics) H Hui-Dong Qian (Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,) X Xiaobai Ma (Department of Nuclear Physics) W Wenyun Yang (Institute of Condensed Matter and Material Physics, School of Physics) X Xiaoxiao Fang (Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,) Q Qing Xu J Jingzhi Han (Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,) H Honglin Du (College of Chemistry and Molecular Engineering, Beijing National Laboratory for Molecular Sciences) J Jinbo Yang (Institute of Condensed Matter and Material Physics, School of Physics) Y Yingchang Yang (Institute of Condensed Matter and Material Physics, School of Physics)

Abstract

The structure, intrinsic magnetic properties, and domain structure of Sm0.7Zr0.3(Fe0.75Co0.25)11.5M0.5 (M = Ti, Mo) compounds were systematically investigated using neutron diffraction, magnetic measurements, magneto-optical Kerr effect, and first-principles calculations. The results demonstrate that the ThMn12-type structure is co-stabilized by substituting Zr for Sm at the 2a site and M for Fe at the 8i site. The effect of M substitution on the electronic band structure can be explained by the rigid band model, where the d–d electron-orbital hybridization between M and Fe leads to a negative effect on the Fe local magnetic moment. Besides, M changes the magnetic anisotropy by altering the electronic density surrounding Sm. Both the compounds exhibit higher Curie temperatures and magnetocrystalline anisotropy fields compared to the well-known Nd2Fe14B magnet, with Tc and μ0Ha reaching 819.3 K and 9.23 T for M = Ti, and 820.0 K and 8.41 T for M = Mo, respectively. The relevant magnetic domain parameters also indicate that these compounds have significant potential for the development of permanent magnet materials.

Article Details

Volume / Issue Vol. 127, Issue 2
Published July 14, 2025
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (12)

S

Shaohua Fan

School of Materials Science and Engineering of Shanxi Normal University & Key Laboratory of Magnetic Molecules and Magnetic Information Materials of Ministry of Education

Z

Zhongchong Lin

Fujian Provincial Key Laboratory of Quantum Manipulation and New Energy Materials, College of Physics and Energy

B

Baochun Wu

State Key Laboratory of Low Dimensional Quantum Physics and Department of Physics

H

Hui-Dong Qian

Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,

X

Xiaobai Ma

Department of Nuclear Physics

W

Wenyun Yang

Institute of Condensed Matter and Material Physics, School of Physics

X

Xiaoxiao Fang

Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,

Q

Qing Xu

J

Jingzhi Han

Institute of Condensed Matter and Material Physics, School of Physics, Peking University 1 , Beijing 100871,

H

Honglin Du

College of Chemistry and Molecular Engineering, Beijing National Laboratory for Molecular Sciences

J

Jinbo Yang

Institute of Condensed Matter and Material Physics, School of Physics

Y

Yingchang Yang

Institute of Condensed Matter and Material Physics, School of Physics