Gapless Andreev bound states in the quantum spin Hall insulator HgTe

Journal Article (2017)
Author(s)

Erwann Bocquillon (Julius-Maximilians-Universität Würzburg)

Russell S. Deacon (RIKEN Center for Emergent Matter Science (CEMS))

Jonas Wiedenmann (Julius-Maximilians-Universität Würzburg)

Philipp Leubner (Julius-Maximilians-Universität Würzburg)

Teunis M. Klapwijk (TU Delft - QN/Klapwijk Lab)

Christoph Brüne (Julius-Maximilians-Universität Würzburg)

Koji Ishibashi (RIKEN Center for Emergent Matter Science (CEMS))

Hartmut Buhmann (Julius-Maximilians-Universität Würzburg)

Laurens W. Molenkamp (Julius-Maximilians-Universität Würzburg)

DOI related publication
https://doi.org/10.1038/nnano.2016.159 Final published version
More Info
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Publication Year
2017
Language
English
Issue number
2
Volume number
12
Pages (from-to)
137-143
Downloads counter
222

Abstract

In recent years, Majorana physics has attracted considerable attention because of exotic new phenomena and its prospects for fault-tolerant topological quantum computation. To this end, one needs to engineer the interplay between superconductivity and electronic properties in a topological insulator, but experimental work remains scarce and ambiguous. Here, we report experimental evidence for topological superconductivity induced in a HgTe quantum well, a 2D topological insulator that exhibits the quantum spin Hall (QSH) effect. The a.c. Josephson effect demonstrates that the supercurrent has a 4π periodicity in the superconducting phase difference, as indicated by a doubling of the voltage step for multiple Shapiro steps. In addition, this response like that of a superconducting quantum interference device to a perpendicular magnetic field shows that the 4π-periodic supercurrent originates from states located on the edges of the junction. Both features appear strongest towards the QSH regime, and thus provide evidence for induced topological superconductivity in the QSH edge states.