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Large anomalous Hall effect induced by weak ferromagnetism in the noncentrosymmetric antiferromagnet CoNb3S6

Hiroaki Tanaka1, Shota Okazaki2, Kenta Kuroda1,*, Ryo Noguchi1,3,4, Yosuke Arai1, Susumu Minami5, Shinichiro Ideta6,†, Kiyohisa Tanaka6, Donghui Lu7 et al.

Makoto Hashimoto7, Viktor Kandyba8, Mattia Cattelan8, Alexei Barinov8, Takayuki Muro9, Takao Sasagawa2,‡, and Takeshi Kondo1,10,§

  • 1Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 2Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama, Kanagawa 226-8503, Japan
  • 3Center for Correlated Electron Systems, Institute for Basic Science, Seoul 08826, Republic of Korea
  • 4Department of Physics and Astronomy, Seoul National University, Seoul 08826, Republic of Korea
  • 5Department of Physics, The University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 6UVSOR Facility, Institute for Molecular Science, Okazaki, Aichi 444-8585, Japan
  • 7Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
  • 8Elettra Sincrotrone Trieste, 34149 Basovizza, Trieste, Italy
  • 9Japan Synchrotron Radiation Research Institute (JASRI), Sayo, Hyogo 679-5198, Japan
  • 10Trans-scale Quantum Science Institute, The University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan

  • *Present address: Graduate School of Advanced Science and Engineering, Hiroshima University, Higashi-hiroshima, Hiroshima 739-8526, Japan; kuroken224@hiroshima-u.ac.jp
  • †Present address: Hiroshima Synchrotron Radiation Center, Hiroshima University, Higashi-hiroshima, Hiroshima 739-0046, Japan.
  • ‡sasagawa@msl.titech.ac.jp
  • §kondo1215@issp.u-tokyo.ac.jp

Phys. Rev. B 105, L121102 – Published 4 March, 2022

DOI: https://doi.org/10.1103/PhysRevB.105.L121102

Abstract

We study the mechanism of the exceptionally large anomalous Hall effect (AHE) in the noncentrosymmetric antiferromagnet CoNb3S6 by angle-resolved photoemission spectroscopy (ARPES) and magnetotransport measurements. From ARPES measurements of CoNb3S6 and its family compounds (FeNb3S6 and NiNb3S6), we find a band dispersion unique to the Co intercalation existing near the Fermi level. We further demonstrate that a slight deficiency of sulfur in CoNb3S6 eliminates the ferromagnetism and the AHE simultaneously while hardly changing the band structure, indicating that the weak ferromagnetism is responsible for the emergence of the large AHE. Based on our results, we propose Weyl points near the Fermi level to cause the large AHE.

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