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与超导体耦合的纳米线量子点中的零偏压异常。

Zero-bias anomaly in a nanowire quantum dot coupled to superconductors.

机构信息

SPSMS, CEA-INAC/UJF-Grenoble 1, 17 rue des Martyrs, 38054 Grenoble Cedex 9, France.

出版信息

Phys Rev Lett. 2012 Nov 2;109(18):186802. doi: 10.1103/PhysRevLett.109.186802. Epub 2012 Oct 31.

Abstract

We studied the low-energy states of spin-1/2 quantum dots defined in InAs/InP nanowires and coupled to aluminum superconducting leads. By varying the superconducting gap Δ with a magnetic field B we investigated the transition from strong coupling Δ << T(K) to weak-coupling Δ >> T(K), where T(K) is the Kondo temperature. Below the critical field, we observe a persisting zero-bias Kondo resonance that vanishes only for low B or higher temperatures, leaving the room to more robust subgap structures at bias voltages between Δ and 2Δ. For strong and approximately symmetric tunnel couplings, a Josephson supercurrent is observed in addition to the Kondo peak. We ascribe the coexistence of a Kondo resonance and a superconducting gap to a significant density of intragap quasiparticle states, and the finite-bias subgap structures to tunneling through Shiba states. Our results, supported by numerical calculations, own relevance also in relation to tunnel-spectroscopy experiments aiming at the observation of Majorana fermions in hybrid nanostructures.

摘要

我们研究了定义在 InAs/InP 纳米线中的自旋为 1/2 的量子点的低能态,并将其与铝超导引线耦合。通过改变超导能隙 Δ 和磁场 B,我们研究了从强耦合 Δ << T(K)到弱耦合 Δ >> T(K)的转变,其中 T(K)是科顿温度。在临界磁场以下,我们观察到持续存在的零偏置科顿共振,只有在低 B 或更高温度下才会消失,这为偏置电压在 Δ 和 2Δ 之间的亚带隙结构留下了空间。对于强且近似对称的隧道耦合,除了科顿峰之外,还观察到约瑟夫森超导电流。我们将科顿共振和超导能隙的共存归因于带隙内准粒子态的密度很大,而有限偏置的亚带隙结构则归因于通过 Shiba 态的隧道。我们的结果得到了数值计算的支持,与旨在观察混合纳米结构中马约拉纳费米子的隧道光谱实验也有关。

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