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Scattering states of a vortex in the proximity-induced superconducting state at the interface of a topological insulator and an s-wave superconductor

机译:在接近引起的超导中的涡旋的散射状态   在拓扑绝缘体和s波的界面处的状态   超导体

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摘要

We consider an isolated vortex in the two-dimensional proximity-inducedsuperconducting state formed at the interface of a three-dimensional strongtopological insulator (TI) and an s-wave superconductor (sSC). Priorcalculations of the bound states of this system famously revealed a zero-energystate that is its own conjugate, a Majorana fermion bound to the vortex core.We calculate, not the bound states, but the scattering states of this system,and ask how the spin-momentum-locked massless Dirac form of the single-particleHamiltonian, inherited from the TI surface, affects the cross section forscattering Bogoliubov quasiparticles from the vortex. As in the case of anordinary superconductor, this is a two-channel problem with the vortex mixingparticle-like and hole-like excitations. And as in the ordinary case, thesame-channel differential cross section diverges in the forward direction dueto the Aharonov-Bohm effect, resulting in an infinite total cross section butfinite transport and skew cross sections. We calculate the transport and skewcross sections numerically, via a partial wave analysis, as a function of bothquasiparticle excitation energy and chemical potential. Novel effects emerge asparticle-like or hole-like excitations are tuned through the Dirac point.
机译:我们考虑在三维强拓扑绝缘体(TI)和s波超导体(sSC)的界面处形成的二维接近感应超导状态下的孤立涡旋。对该系统的束缚态的事先计算著名地揭示了零能量态是其自身的共轭物,即绑定到涡旋核的马约拉那费米子。我们不是计算束缚态,而是计算该系统的散射态,并询问自旋如何TI表面继承的单粒子哈密顿的动量锁无质量Dirac形式影响了Bogoliubov准粒子从涡旋散射的截面。与普通的超导体一样,这是一个涡旋混合了类粒子和类空穴激励的两通道问题。与通常情况一样,相同通道的微分横截面由于Aharonov-Bohm效应而在正向方向上发散,从而导致无限大的总横截面,有限的传输和偏斜横截面。我们通过局部波分析,计算了准截面激发能和化学势的函数,计算了传输截面和斜截面的数值。通过狄拉克点调整类粒子或类孔激发时会出现新颖的效果。

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    Durst, Adam C.;

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  • 年度 2016
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  • 入库时间 2022-08-20 21:10:13

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