Unusual Anomalous Hall Resistivities of CuCr<sub>2</sub>S<sub>4</sub>, Cu<sub>0.5</sub>Zn<sub>0.5</sub>Cr<sub>2</sub>Se<sub>4</sub> and Cr<sub>3</sub>Te<sub>4</sub>

  • Oda Keisuke
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602
  • Yoshii Shunsuke
    CREST, Japan Science and Technology Corporation (JST)
  • Yasui Yukio
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 CREST, Japan Science and Technology Corporation (JST)
  • Ito Masafumi
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 CREST, Japan Science and Technology Corporation (JST)
  • Ido Takahiko
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602
  • Ohno Youhei
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602
  • Kobayashi Yoshiaki
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 CREST, Japan Science and Technology Corporation (JST)
  • Sato Masatoshi
    Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 CREST, Japan Science and Technology Corporation (JST)

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タイトル別名
  • Unusual Anomalous Hall Resistivities of CuCr2S4, Cu0.5Zn0.5Cr2Se4 and Cr3Te4.

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説明

Hall resistivities ρH, the magnetizations M and the magnetoresistances Δρ have been measured as functions of the applied magnetic field H in the wide temperature range for ferromagnetic systems of CuCr2S4, Cu0.5Zn0.5Cr2Se4 and Cr3Te4, which are considered to have non-trivial spin structures below the temperature Tm. For CuCr2S4 and Cr3Te4, the Hall resistivities have been found to deviate from the ordinary expression ρH=R0H+4π RsM below Tm, where R0 and Rs are the ordinary and anomalous Hall coefficients, respectively. The sign change of Rs with T has also been observed for all the systems. These behaviors are discussed in relation to their possibly non-trivial magnetic structures.

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