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Two-dimensional time-reversal-invariant topological superconductivity in a doped quantum spin-Hall insulator

机译:掺杂量子自旋霍尔绝缘体中的二维时不变不变拓扑超导

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摘要

Time-reversal-invariant topological superconductors have a full paring gap in the bulk and gapless Majorana states at the edge or on the surface. Here, we theoretically propose topological superconductivity in a doped quantum spin-Hall insulator. We study the pairing symmetry of a doped two-dimensional tin film within a two-orbital model, and find that a novel spin-triplet pairing is favored when the interorbital attractive interaction is stronger than the intraorbital interaction. We propose that a doped tin film is a good candidate for a 2d topological superconductor. Edge channels are studied in a tight-binding model numerically. Finally, we discuss the robustness of topological superconductivity in two-dimensional tin films by comparing to 3d superconductivity in bulk tin.
机译:时变不变的拓扑超导体在边缘或表面的体态和无间隙的马里亚纳状态中具有完全的配对间隙。在这里,我们从理论上提出了掺杂量子自旋霍尔绝缘体中的拓扑超导性。我们研究了在两轨道模型中掺杂的二维锡膜的配对对称性,发现当轨道间吸引相互作用强于轨道内相互作用时,新型自旋三重态配对受到青睐。我们建议掺杂锡膜是2D拓扑超导体的理想选择。在紧密绑定模型中对边缘通道进行了数值研究。最后,通过与块状锡中的3d超导比较,我们讨论了二维锡膜中拓扑超导的鲁棒性。

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  • 来源
    《Physical review 》 |2014年第5期| 054503.1-054503.5| 共5页
  • 作者单位

    Department of Physics, McCullough Building, Stanford University, Stanford, California 94305-4045, USA;

    Department of Physics, McCullough Building, Stanford University, Stanford, California 94305-4045, USA;

    Department of Physics, McCullough Building, Stanford University, Stanford, California 94305-4045, USA;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    pairing symmetries (other than s-wave); quantum hall effects;

    机译:配对对称性(s波除外);量子霍尔效应;

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