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Negative Te spin polarization responsible for ferromagnetic order in the doped topological insulator V_(0.04)(Sb_(1-x)Bi_x)_(1.96)Te_3

机译:负Te自旋极化负责掺杂拓扑绝缘体V_(0.04)(Sb_(1-x)Bi_x)_(1.96)Te_3中的铁磁序

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摘要

Ferromagnetic topological insulators have emerged as a promising platform for quantum anomalous Hall (QAH) effect with a dissipationless edge transport. However, the observation of QAH effect has so far been restricted to extremely low temperatures. We investigate the microscopic origin of ferromagnetism coupled with topological insulators in vanadium-doped (Sb, Bi)(2)Te-3 employing the x-ray magnetic circular dichroism, angle-resolved two-photon photoemission spectroscopy, combined with first-principles calculations. We found a negative spin polarization, and thus an antiparallel magnetic moment at the Te site with respect to that of the vanadium dopants, which plays the key role in the ferromagnetic order. We ascribe it to the hybridization between Te p and V d majority spin states at the Fermi energy (E-F), being supported by a Zener-type p-d exchange interaction scenario. The substitution of Bi at the Sb site suppresses the bulk ferromagnetism by introducing extra electron carriers in the majority spin channel of Te p states that compensates the antiparallel magnetic moment on the Te site. Our findings reveal important clues to designing magnetic topological insulators with higher Curie temperature that work under ambient conditions.
机译:铁磁拓扑绝缘体已成为具有无耗散边缘传输的量子异常霍尔(QAH)效应的有前途的平台。然而,迄今为止,对QAH效应的观察仅限于极低的温度。我们研究了使用X射线磁性圆二色性,角度分辨双光子光发射光谱法结合第一性原理计算的钒掺杂(Sb,Bi)(2)Te-3中铁磁与拓扑绝缘体耦合的微观起源。我们发现负自旋极化,从而在Te位置发现相对于钒掺杂剂的反平行磁矩,这在铁磁有序中起关键作用。我们将其归因于Zener型p-d交换相互作用场景支持的费米能量(E-F)下Te p和V d多数自旋态之间的杂化。通过在Te p态的大部分自旋通道中引入额外的电子载流子,以补偿Te点上的反平行磁矩,在Sb位点上Bi的取代抑制了整体铁磁性。我们的发现揭示了设计在环境条件下工作的居里温度更高的磁性拓扑绝缘子的重要线索。

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  • 来源
    《Physical review》 |2019年第14期|144413.1-144413.7|共7页
  • 作者单位

    Chinese Acad Sci, Shanghai Inst Microsyst & Informat Technol, State Key Lab Funct Mat Informat, Shanghai 200050, Peoples R China|Chinese Acad Sci, Ctr Excellence Superconducting Elect CENSE, Shanghai 200050, Peoples R China;

    Chinese Acad Sci, Shanghai Inst Microsyst & Informat Technol, State Key Lab Funct Mat Informat, Shanghai 200050, Peoples R China|Chinese Acad Sci, Ctr Excellence Superconducting Elect CENSE, Shanghai 200050, Peoples R China|Univ Chinese Acad Sci, Beijing 100049, Peoples R China;

    ShanghaiTech Univ, Sch Phys Sci & Technol, Shanghai 201210, Peoples R China;

    Chinese Acad Sci, Shanghai Inst Microsyst & Informat Technol, State Key Lab Funct Mat Informat, Shanghai 200050, Peoples R China|Chinese Acad Sci, Ctr Excellence Superconducting Elect CENSE, Shanghai 200050, Peoples R China|ShanghaiTech Univ, Sch Phys Sci & Technol, Shanghai 201210, Peoples R China;

    Japan Atom Energy Agcy, Mat Sci Res Ctr, Mikazuki, Hyogo 6795148, Japan;

    Japan Atom Energy Agcy, Mat Sci Res Ctr, Mikazuki, Hyogo 6795148, Japan;

    Hiroshima Univ, Grad Sch Sci, 1-3-1 Kagamiyama, Higashihiroshima 7398526, Japan;

    Hiroshima Univ, Grad Sch Sci, 1-3-1 Kagamiyama, Higashihiroshima 7398526, Japan;

    Hiroshima Univ, Grad Sch Sci, 1-3-1 Kagamiyama, Higashihiroshima 7398526, Japan;

    Univ Tokyo, ISSP, 5-1-5 Kashiwa Ha, Chiba 2778581, Japan;

    Univ Tokyo, ISSP, 5-1-5 Kashiwa Ha, Chiba 2778581, Japan;

    Hiroshima Univ, Grad Sch Sci, 1-3-1 Kagamiyama, Higashihiroshima 7398526, Japan;

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