4.8 Article

Intrinsic hard magnetism and thermal stability of a ThMn12-type permanent magnet

Journal

NPJ COMPUTATIONAL MATERIALS
Volume 8, Issue 1, Pages -

Publisher

NATURE PORTFOLIO
DOI: 10.1038/s41524-022-00821-8

Keywords

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Funding

  1. Future Materials Discovery Program [2016M3D1A1027831]
  2. National Research Foundation of Korea (NRF) - Ministry of Science and ICT [2020R1F1A1067589]
  3. Korea Institute of Energy Technology Evaluation and Planning (KETEP) - Korea government (MOTIE) [20192010106850]
  4. National Research Foundation of Korea [2020R1F1A1067589] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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In this study, it was theoretically demonstrated that simple metal substitutional atoms not only stabilized certain phases but also improved their magnetic properties. Furthermore, these atoms also improved the single-domain size of the particles. The results were explained by the strong spin-orbit coupling and orbital angular momentum of the Sm 4f-electron orbitals.
Herein, we theoretically demonstrate that simple metal (Ga and Al) substitutional atoms, rather than the conventional transition metal substitutional elements, not only stabilize the ThMn12-type SmFe12 and Sm(Fe,Co)(12) phases thermodynamically but also further improve their intrinsic magnetic properties such that they are superior to those of the widely investigated SmFe11Ti and Sm(Fe,Co)(11)Ti magnets, and even to the state-of-the-art permanent magnet Nd2Fe14B. More specifically, the quaternary Sm(Fe,Co,Al)(12) phase has the highest uniaxial magnetocrystalline anisotropy (MCA) of about 8 MJ m(-3), anisotropy field of 18.2 T, and hardness parameter of 2.8 at room temperature and a Curie temperature of 764 K. Simultaneously, the Al and Ga substitutional atoms improve the single-domain size of the Sm(Fe,Co)(12) grains by nearly a factor of two. Numerical results of MCA and MCA-driven hard magnetic properties can be described by the strong spin-orbit coupling and orbital angular momentum of the Sm 4f-electron orbitals.

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