Spontaneous Hall effect induced by altermagnetic order at room temperature

ORAL

Abstract

Today, magnetic information is mostly stored in ferromagnets, where the up and down spin states are distinguishable due to time-reversal symmetry breaking. In these two states, electric current induces the opposite sign of transverse voltage in proportion to magnetization (anomalous Hall effect), and this phenomenon has been widely used for electrical readout of the up and down spin states in ferromagnets. In contrast, the aforementioned functions cannot be expected in conventional antiferromagnets with collinear antiparallel (up-down) spin configuration, because of its macroscopic time-reversal symmetry (TRS) and lack of macroscopic magnetization. According to recent theories, however, it has been predicted that such a collinear antiferromagnetic order can often host sizable spontaneous Hall effect even without net magnetization or external magnetic field, when combined with a crystal lattice with appropriate symmetry. Such a TRS-broken collinear antiferromagnet is often termed “altermagnet”.

In this talk, I report the experimental observation of spontaneous Hall effect in a collinear antiferromagnet at room temperature [1]. In this compound, the up-down and down-up spin states induce the opposite sign of spontaneous Hall effect. Our detailed analysis suggests that the observed spontaneous Hall signal does not reflect magnetization, but rather originates from the fictitious magnetic field associated with TRS-broken antiferromagnetic order. The present results pave the way for the electrical reading and possible writing of the up-down and down-up spin states in conductive systems at room temperature, which suggests that TRS-broken collinear antiferromagnets may serve as a unique information medium to realize nontrivial spintronic responses with vanishingly small magnetization.

[1] R. Takagi, R. Hirakida, Y. Settai, R. Oiwa, H. Takagi, A. Kitaori, K. Yamauchi, H. Inoue, J. Yamaura, D. Nishio-Hamane, S. Itoh, S. Aji, H. Saito, T. Nakajima, T. Nomoto, R. Arita, S. Seki, Nature Materials (in press)

*This work was supported by KAKENHI (19H05825, 20K21067, 21H04990, 21K13876, 21K18595, 21H04437, 22H04965, 24H02235 and 24K00579) from JSPS, PRESTO (JPMJPR18L5, JPMJPR20B4, JPMJPR20L7, and JPMJPR23Q3) and CREST (JPMJCR23O4) from JST.

Publication: R. Takagi, R. Hirakida, Y. Settai, R. Oiwa, H. Takagi, A. Kitaori, K. Yamauchi, H. Inoue, J. Yamaura, D. Nishio-Hamane, S. Itoh, S. Aji, H. Saito, T. Nakajima, T. Nomoto, R. Arita, S. Seki, Nature Materials (in press)

Presenters

  • Shinichiro Seki

    • Univ of Tokyo

Authors

  • Shinichiro Seki

    • Univ of Tokyo
  • Rina Takagi

    • University of Tokyo
  • Ryosuke Hirakida

    • University of Tokyo
  • Yuki Settai

    • Univ. of Tokyo
    • University of Tokyo
  • Rikuto Oiwa

    • RIKEN
  • Hirotaka Takagi

    • University of Tokyo
  • Aki Kitaori

    • Univ of Tokyo
  • Kensei Yamauchi

    • University of Tokyo
  • Hiroki Inoue

    • University of Tokyo
  • Jun-ichi Yamaura

    • Institute for Solid State Physics, University of Tokyo
    • University of Tokyo
  • Daisuke Nishio-Hamane

    • University of Tokyo
    • Univ of Tokyo
  • Shinichi Itoh

    • Institute of Materials Structure Science, KEK
    • University of Tokyo
    • High Energy Accelerator Research Organization
  • Seno Aji

    • University of Tokyo
  • Hiraku Saito

    • Institute for Solid State Physics (ISSP)
    • University of Tokyo
  • Taro Nakajima

    • The Institute for Solid State Physics, University of Tokyo
    • Institute for Solid State Physics (ISSP)
    • University of Tokyo
  • Takuya Nomoto

    • Univ of Tokyo
    • Tokyo Metropolitan University
    • Tokyo Metropolitan Univ.
  • Ryotaro Arita

    • Univ of Tokyo
    • Univ. of Tokyo, RIKEN CEMS