Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan.
Department of Physics, Stockholm University, Se-106 91 Stockholm, Sweden.
Phys Rev Lett. 2013 Mar 15;110(11):117002. doi: 10.1103/PhysRevLett.110.117002. Epub 2013 Mar 12.
We study theoretically the proximity effect of a one-dimensional metallic quantum wire (in the absence of spin-orbit interaction) lying on top of an unconventional superconductor. Three different material classes are considered as a substrate: (i) a chiral superconductor in class D with broken time-reversal symmetry and a class DIII superconductor (ii) with and (iii) without a nontrivial Z(2) number. Interestingly, we find degenerate zero energy Majorana bound states at both ends of the wire for all three cases. They are unstable against spin-orbit interaction in case (i), while they are topologically protected by time-reversal symmetry in cases (ii) and (iii). Remarkably, we show that nonlocal spin correlations between the two ends of the wire can be simply controlled by a gate potential in our setup.
我们从理论上研究了位于非常规超导体之上的一维金属量子线(无自旋轨道相互作用)的近邻效应。我们考虑了三种不同的材料作为衬底:(i)具有破坏时间反演对称性的 D 类手性超导体和具有和(ii)不具有非平凡 Z(2)数的 DIII 超导体。有趣的是,我们发现对于所有三种情况,在线的两端都存在简并的零能马约拉纳束缚态。对于情况(i),它们对自旋轨道相互作用不稳定,而对于情况(ii)和(iii),它们则受到时间反演对称性的拓扑保护。值得注意的是,我们表明,在我们的设置中,通过栅极电势可以简单地控制线两端之间的非局域自旋相关性。