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    Spin-polarized electronic structure of tetragonally distorted FeCo thin films on Rh(001) exhibiting perpendicular magnetic anisotropy

    Kaori Kunitomo1, Kazuki Sumida2,*, Koji Miyamoto2, and Taichi Okuda2,3,4,†

    • 1Graduate School of Advanced Science and Engineering, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima 739-8526, Japan
    • 2Research Institute for Synchrotron Radiation Science (HiSOR), Hiroshima University, 2-313 Kagamiyama, Higashi-Hiroshima 739-0046, Japan
    • 3International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM2), Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima 739-8526, Japan
    • 4Research Institute for Semiconductor Engineering (RISE), Hiroshima University, 1-4-2 Kagamiyama, Higashi-Hiroshima 739-8527, Japan

    • *Contact author: sumidak1126@hiroshima-u.ac.jp
    • †Contact author: okudat@hiroshima-u.ac.jp

    Phys. Rev. Materials 9, 064407 – Published 12 June, 2025

    DOI: https://doi.org/10.1103/rdfk-lnzl

    Abstract

    A tetragonally distorted FeCo alloy is a ferromagnetic material exhibiting perpendicular magnetic anisotropy (PMA) with a large saturation magnetization. Theoretical investigations have proposed that PMA in FeCo is caused by the hybridization of the certain orbitals near the Fermi energy (EF) in the minority-spin channel, but experimental verification of the electronic structure has yet to be performed. Here, using spin- and angle-resolved photoemission spectroscopy (SARPES) combined with first-principles calculations, we investigated the spin- and orbital-dependent electronic structure of tetragonally distorted FeCo films on a Rh(001) substrate. Our SARPES results show clear out-of-plane spin polarization at room temperature. Furthermore, by considering the matrix element effect and experimental geometry, we revealed that the spin-polarized bands around EF of FeCo films possessing PMA are mainly composed of minority-spin dxy and dx2−y2 orbitals. Our findings provide deep insight into the emergence of PMA in rare-element-free magnetic materials.

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