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掺杂石墨烯中拟议的手性 d 波超导态中的边缘性质和马约拉纳费米子。

Edge properties and Majorana fermions in the proposed chiral d-wave superconducting state of doped graphene.

机构信息

Department of Physics and Astronomy, Uppsala University, Box 516, S-751 20 Uppsala, Sweden.

出版信息

Phys Rev Lett. 2012 Nov 9;109(19):197001. doi: 10.1103/PhysRevLett.109.197001. Epub 2012 Nov 7.

Abstract

We investigate the effect of edges on the intrinsic d-wave superconducting state in graphene doped close to the van Hove singularity. While the bulk is in a chiral d(x(2)-y(2)) + id(xy) state, the order parameter at any edge is enhanced and has d(x(2)-y(2))-symmetry, with a decay length strongly increasing with weakening superconductivity. No graphene edge is pair breaking for the d((x(2)-y{2)) state, and there are no localized zero-energy edge states. We find two chiral edge modes which carry a spontaneous, but not quantized, quasiparticle current related to the zero-energy momentum. Moreover, for realistic values of the Rashba spin-orbit coupling, a Majorana fermion appears at the edge when tuning a Zeeman field.

摘要

我们研究了边缘对在范霍夫奇点附近掺杂的石墨烯本征 d 波超导态的影响。虽然体相处于手性 d(x(2)-y(2)) + id(xy) 态,但任何边缘的序参量都会增强,并且具有 d(x(2)-y(2)) 对称性,其衰减长度随着超导性的减弱而强烈增加。对于 d((x(2)-y{2)) 态,没有石墨烯边缘会破坏对,也没有局域的零能边缘态。我们发现了两个手性边缘模式,它们携带与零能动量相关的自发但非量子化的准粒子电流。此外,对于现实的拉什巴自旋轨道耦合值,当调节塞曼场时,马约拉纳费米子出现在边缘。

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