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利用 ω-SQUIPT 对约瑟夫森拓扑材料进行相位工程。

The ω-SQUIPT as a tool to phase-engineer Josephson topological materials.

机构信息

NEST, Istituto Nanoscienze-CNR and Scuola Normale Superiore, Piazza S. Silvestro 12, I-56127 Pisa, Italy.

Centro de Fisica de Materiales (CFM-MPC), Centro Mixto CSIC-UPV/EHU, Manuel de Lardizabal 5, E-20018 San Sebastian, Spain.

出版信息

Nat Nanotechnol. 2016 Dec;11(12):1055-1059. doi: 10.1038/nnano.2016.157. Epub 2016 Sep 12.

DOI:10.1038/nnano.2016.157
PMID:27618256
Abstract

Multi-terminal superconducting Josephson junctions based on the proximity effect offer the opportunity to tailor non-trivial quantum states in nanoscale weak links. These structures can realize exotic topologies in several dimensions, for example, artificial topological superconductors that are able to support Majorana bound states, and pave the way to emerging quantum technologies and future quantum information schemes. Here we report the realization of a three-terminal Josephson interferometer based on a proximized nanosized weak link. Our tunnelling spectroscopy measurements reveal transitions between gapped (that is, insulating) and gapless (conducting) states that are controlled by the phase configuration of the three superconducting leads connected to the junction. We demonstrate the topological nature of these transitions: a gapless state necessarily occurs between two gapped states of different topological indices, in much the same way that the interface between two insulators of different topologies is necessarily conducting. The topological numbers that characterize such gapped states are given by superconducting phase windings over the two loops that form the Josephson interferometer. As these gapped states cannot be transformed to one another continuously without passing through a gapless condition, they are topologically protected. The same behaviour is found for all of the points of the weak link, confirming that this topology is a non-local property. Our observation of the gapless state is pivotal for enabling phase engineering of different and more sophisticated artificial topological materials.

摘要

基于近邻效应的多端超导约瑟夫森结为在纳米级弱连接中定制非平凡量子态提供了机会。这些结构可以在几个维度上实现奇异拓扑,例如能够支持马约拉纳束缚态的人工拓扑超导体,并为新兴量子技术和未来量子信息方案铺平道路。在这里,我们报告了基于近邻化纳米级弱连接的三端约瑟夫森干涉仪的实现。我们的隧道谱测量揭示了由连接到结的三个超导引线的相位配置控制的带隙(即绝缘)和无带隙(传导)状态之间的转变。我们证明了这些转变的拓扑性质:在具有不同拓扑指数的两个带隙状态之间必然存在无带隙状态,这与不同拓扑绝缘体之间的界面必然是传导的方式非常相似。这些带隙状态的拓扑数由形成约瑟夫森干涉仪的两个环路的超导相位缠绕给出。由于这些带隙状态不能在不经过无带隙条件的情况下相互连续转换,因此它们是拓扑保护的。在弱连接的所有点都发现了相同的行为,这证实了这种拓扑是一种非局部性质。我们对无带隙状态的观察对于实现不同和更复杂的人工拓扑材料的相位工程至关重要。

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