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    Piezomagnetic effect in 5d transition metal oxides Y2Ir2O7 and Cd2Os2O7 with all-in/all-out magnetic order

    Hiroki Nanjo1,*, Yoshinori Imai1,2, Takuya Aoyama3,4, Jun-ichi Yamaura5, and Kenya Ohgushi1

    • 1Department of Physics, Graduate School of Science, Tohoku University, 6-3 Aramaki-Aoba, Aoba-ku, Sendai, Miyagi 980-8578, Japan
    • 2Institute for Excellence in Higher Education, Tohoku University, 41 Kawauchi, Aoba-ku, Sendai, Miyagi 980-8576, Japan
    • 3Department of Quantum Matter, Graduate School of Advanced Science and Engineering, Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima, Hiroshima 739-8530, Japan
    • 4International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM2), Hiroshima University, 1-3-1 Kagamiyama, Higashi-Hiroshima 739-8531, Japan
    • 5Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan

    • *Contact author: nanjo.hiroki.s7@dc.tohoku.ac.jp

    Phys. Rev. B 113, 174434 – Published 21 May, 2026

    DOI: https://doi.org/10.1103/7591-1lgx

    Abstract

    We investigate the piezomagnetic effect in pyrochlore-type oxides Y2Ir2O7 and Cd2Os2O7, which exhibit a noncoplanar magnetic structure called the all-in/all-out antiferromagnetic order at low temperatures. The all-in/all-out magnetic order can be viewed as a ferroic order of the xyz-type magnetic octupoles. In both oxide materials, we observe a linear increase in magnetization with applied stress. We then estimate the powder-averaged piezomagnetic tensor at the lowest measured temperature 10 K to be Q=6.36×10−6 μB/Ir/MPa for Y2Ir2O7 and Q=3.83×10−7 μB/Os/MPa for Cd2Os2O7. We discuss the microscopic mechanism of the piezomagnetic effect based on the stress-induced modification of the g-tensor anisotropy and Dzyaloshinskii-Moriya interactions. This work supports further development of piezomagnetic materials using magnetic multipoles.

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