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直拉法生长的CoSi单晶中的舒布尼科夫-德哈斯振荡和德哈斯-范阿尔芬振荡

Shubnikov-de Haas and de Haas-van Alphen oscillations in Czochralski grown CoSi single crystal.

作者信息

Sasmal Souvik, Dwari Gourav, Baran Maity Bishal, Saini Vikas, Thamizhavel A, Mondal Rajib

机构信息

Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India.

UGC-DAE Consortium for Scientific Research, Kolkata Centre, Bidhannagar, Kolkata 700 106, India.

出版信息

J Phys Condens Matter. 2022 Aug 24;34(42). doi: 10.1088/1361-648X/ac8960.

Abstract

Anisotropic transport, Shubnikov-de Haas (SdH), and de Haas-van Alphen (dHvA) quantum oscillations studies are reported on a high-quality CoSi single crystal grown by the Czochralski method. Temperature-dependent resistivities indicate the dominating electron-electron scattering. Magnetoresistance (MR) at 2 K reaches 610% forI ∥ [111]andB ∥ [011-], whereas it is 500% forI ∥ [011-] andB ∥ [111]. A negative slope in field-dependent Hall resistivity suggests electrons are the majority carriers. The carrier concentration extracted from Hall conductivity indicates no electron-hole compensation. In 3D CoSi, the electron transport lifetime is found to be approximately in the same order as the quantum lifetime, whereas in 2electron gas the long-range scattering drives the transport life much larger than the quantum lifetime. From MR and Hall SdH oscillations, the effective masses and Dingle temperatures have been calculated. The dHvA oscillation reveals three frequencies at 18 T (), 558 T () and 663 T (), whereas, SdH oscillation results in only two frequenciesand. Thefrequency observed in dHvA oscillation is a tiny hole pocket at the Γ point.

摘要

报道了对通过提拉法生长的高质量CoSi单晶进行的各向异性输运、舒布尼科夫-德哈斯(SdH)和德哈斯-范阿尔芬(dHvA)量子振荡研究。与温度相关的电阻率表明电子-电子散射起主导作用。在2 K时,当电流I∥[111]且磁场B∥[011-]时,磁电阻(MR)达到610%,而当电流I∥[011-]且磁场B∥[111]时,磁电阻为500%。磁场依赖的霍尔电阻率的负斜率表明电子是多数载流子。从霍尔电导率提取的载流子浓度表明不存在电子-空穴补偿。在三维CoSi中,发现电子输运寿命与量子寿命大致处于同一量级,而在二维电子气中,长程散射使得输运寿命远大于量子寿命。通过磁电阻和霍尔SdH振荡,计算出了有效质量和丁格尔温度。dHvA振荡在18 T()、558 T()和663 T()处显示出三个频率,而SdH振荡仅产生两个频率和。在dHvA振荡中观察到的频率对应于Γ点处的一个微小空穴口袋。

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