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掺杂拓扑绝缘体中超导体涡旋两端的马约拉纳模。

Majorana modes at the ends of superconductor vortices in doped topological insulators.

机构信息

Department of Physics, University of California, Berkeley, California 94720, USA.

出版信息

Phys Rev Lett. 2011 Aug 26;107(9):097001. doi: 10.1103/PhysRevLett.107.097001. Epub 2011 Aug 22.

Abstract

Recent experiments have observed bulk superconductivity in doped topological insulators. Here we ask whether vortex Majorana zero modes, previously predicted to occur when s-wave superconductivity is induced on the surface of topological insulators, survive in these doped systems with metallic normal states. Assuming inversion symmetry, we find that they do but only below a critical doping. The critical doping is tied to a topological phase transition of the vortex line, at which it supports gapless excitations along its length. The critical point depends only on the vortex orientation and a suitably defined SU(2) Berry phase of the normal state Fermi surface. By calculating this phase for available band structures we determine that superconducting p-doped Bi(2)Te(3), among others, supports vortex end Majorana modes. Surprisingly, superconductors derived from topologically trivial band structures can support Majorana modes too.

摘要

最近的实验观察到掺杂拓扑绝缘体中的体超导电性。在这里,我们想问一下,当 s 波超导性诱导在拓扑绝缘体的表面上时,先前预测的涡旋马约拉纳零模是否存在于这些掺杂系统的金属正常状态中。假设存在反转对称性,我们发现它们确实存在,但仅在临界掺杂以下。临界掺杂与涡旋线的拓扑相变有关,在此相变中,它支持沿着其长度的无能隙激发。临界点仅取决于涡旋的方向和正常状态费米面的适当定义的 SU(2)贝里相位。通过为可用的能带结构计算这个相位,我们确定超导 p 掺杂 Bi(2)Te(3)等支持涡旋端马约拉纳模。令人惊讶的是,源自拓扑平凡能带结构的超导体也可以支持马约拉纳模。

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