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Anomalous transverse response of Co_2MnGa and universality of the room-temperature α_(ij)~A/σ_(ij)~A ratio across topological magnets

机译:Co_2mnga的异常横向响应和室温α_(ij)〜a /Σ_(ij)跨拓扑磁体的比率

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摘要

The off-diagonal (electric, thermal, and thermoelectric) transport coefficients of a solid can acquire an anomalous component due to the nontrivial topology of the Bloch waves. We present a study of the anomalous Hall effect (AHE), anomalous Nernst effect (ANE), and thermal Hall effect in the Heusler-Weyl ferromagnet Co_2MnGa. The anomalous Wiedemann-Franz law, linking electric and thermal responses, was found to be valid over the whole temperature window. This indicates that the AHE has an intrinsic origin and the Berry spectrum is smooth in the immediate vicinity of the Fermi level. We extract α_(ij)~A from our ANE data and find that the α_(ij)~A/σ_(ij)~A ratio approaches k_B/e at room temperature. Scrutinizing all topological magnets previously explored, we observe that this ratio is a sizable fraction of k_B/e at room temperature. We provide a rough explanation for this feature by arguing that the two anomalous transverse coefficients depend on universal constants, the Berry curvature averaged over a window set by either the Fermi wavelength (for Hall) or the de Broglie thermal length (for Nernst). The universal scaling indicates that the widths of the two windows approaches each other at room temperature.
机译:由于光伏波的非血管拓扑结构,固体的截止对角线(电动,热和热电)传送系数可以获取异常部件。我们展示了Heusler-Weyl Ferromagnet Co_2mnga中的异常霍尔效应(AHE),异常的内部效应(ANE),热霍尔效应。发现有异常的Wiedemann-Franz定律,连接电动和热响应,在整个温度窗口上有效。这表明AHE具有内在原点,并且浆液光谱在费米水平附近平滑。我们从我们的ANE数据中提取α_(IJ)〜A,发现α_(ij)〜a /σ_(ij)〜a比率在室温下接近k_b / e。仔细检查先前探索的所有拓扑磁铁,我们观察到该比率在室温下k_b / e的相当大。我们通过争论两个异常的横向系数取决于通用常数,对该特征提供了粗略的解释,替代通用常数,浆果曲率在由Fermi波长(对于霍尔)或DE Broglie热长(对于NERNST)设置的窗口上平均。通用缩放表示两个窗口的宽度在室温下彼此接近。

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  • 来源
    《Physical review》 |2020年第18期|180404.1-180404.5|共5页
  • 作者单位

    Wuhan National High Magnetic Field Center School of Physics Huazhong University of Science and Technology Wuhan 430074 China Laboratoire de Physique Et Etude des Materiaux (UPMC-CNRS) ESPCI Paris PSL Research University 75005 Paris France;

    Wuhan National High Magnetic Field Center School of Physics Huazhong University of Science and Technology Wuhan 430074 China Laboratoire de Physique Et Etude des Materiaux (UPMC-CNRS) ESPCI Paris PSL Research University 75005 Paris France;

    Wuhan National High Magnetic Field Center School of Physics Huazhong University of Science and Technology Wuhan 430074 China;

    Institute for Solid State Physics University of Tokyo Kashiwa Chiba 277-8581 Japan Department of Physics University of Tokyo Hongo Bunkyo-ku Tokyo 113-0033 Japan CREST Japan Science and Technology Agency (JST) 4-1-8 Honcho Kawaguchi Saitama 332-0012 Japan;

    Institute for Solid State Physics University of Tokyo Kashiwa Chiba 277-8581 Japan Department of Physics University of Tokyo Hongo Bunkyo-ku Tokyo 113-0033 Japan CREST Japan Science and Technology Agency (JST) 4-1-8 Honcho Kawaguchi Saitama 332-0012 Japan;

    JEIP USR 3573 CNRS College de France PSL Research University 11 Place Marcelin Berthelot 75231 Paris Cedex 05 France;

    Institute for Solid State Physics University of Tokyo Kashiwa Chiba 277-8581 Japan Department of Physics University of Tokyo Hongo Bunkyo-ku Tokyo 113-0033 Japan CREST Japan Science and Technology Agency (JST) 4-1-8 Honcho Kawaguchi Saitama 332-0012 Japan;

    Wuhan National High Magnetic Field Center School of Physics Huazhong University of Science and Technology Wuhan 430074 China;

    Wuhan National High Magnetic Field Center School of Physics Huazhong University of Science and Technology Wuhan 430074 China;

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