Topological Superconductivity in a Planar Josephson Junction

We consider a two-dimensional electron gas with strong spin-orbit coupling contacted by two superconducting leads, forming a Josephson junction. We show that in the presence of an in-plane Zeeman field, the quasi-one-dimensional region between the two superconductors can support a topological superc...

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Main Authors: Falko Pientka, Anna Keselman, Erez Berg, Amir Yacoby, Ady Stern, Bertrand I. Halperin
Format: Article
Language:English
Published: American Physical Society 2017-05-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.7.021032
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spelling doaj-bd8338b64ff746a9bf3a780fa3da45ac2020-11-24T23:59:30ZengAmerican Physical SocietyPhysical Review X2160-33082017-05-017202103210.1103/PhysRevX.7.021032Topological Superconductivity in a Planar Josephson JunctionFalko PientkaAnna KeselmanErez BergAmir YacobyAdy SternBertrand I. HalperinWe consider a two-dimensional electron gas with strong spin-orbit coupling contacted by two superconducting leads, forming a Josephson junction. We show that in the presence of an in-plane Zeeman field, the quasi-one-dimensional region between the two superconductors can support a topological superconducting phase hosting Majorana bound states at its ends. We study the phase diagram of the system as a function of the Zeeman field and the phase difference between the two superconductors (treated as an externally controlled parameter). Remarkably, at a phase difference of π, the topological phase is obtained for almost any value of the Zeeman field and chemical potential. In a setup where the phase is not controlled externally, we find that the system undergoes a first-order topological phase transition when the Zeeman field is varied. At the transition, the phase difference in the ground state changes abruptly from a value close to zero, at which the system is trivial, to a value close to π, at which the system is topological. The critical current through the junction exhibits a sharp minimum at the critical Zeeman field and is therefore a natural diagnostic of the transition. We point out that in the presence of a symmetry under a mirror reflection followed by time reversal, the system belongs to a higher symmetry class, and the phase diagram as a function of the phase difference and the Zeeman field becomes richer.http://doi.org/10.1103/PhysRevX.7.021032
collection DOAJ
language English
format Article
sources DOAJ
author Falko Pientka
Anna Keselman
Erez Berg
Amir Yacoby
Ady Stern
Bertrand I. Halperin
spellingShingle Falko Pientka
Anna Keselman
Erez Berg
Amir Yacoby
Ady Stern
Bertrand I. Halperin
Topological Superconductivity in a Planar Josephson Junction
Physical Review X
author_facet Falko Pientka
Anna Keselman
Erez Berg
Amir Yacoby
Ady Stern
Bertrand I. Halperin
author_sort Falko Pientka
title Topological Superconductivity in a Planar Josephson Junction
title_short Topological Superconductivity in a Planar Josephson Junction
title_full Topological Superconductivity in a Planar Josephson Junction
title_fullStr Topological Superconductivity in a Planar Josephson Junction
title_full_unstemmed Topological Superconductivity in a Planar Josephson Junction
title_sort topological superconductivity in a planar josephson junction
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2017-05-01
description We consider a two-dimensional electron gas with strong spin-orbit coupling contacted by two superconducting leads, forming a Josephson junction. We show that in the presence of an in-plane Zeeman field, the quasi-one-dimensional region between the two superconductors can support a topological superconducting phase hosting Majorana bound states at its ends. We study the phase diagram of the system as a function of the Zeeman field and the phase difference between the two superconductors (treated as an externally controlled parameter). Remarkably, at a phase difference of π, the topological phase is obtained for almost any value of the Zeeman field and chemical potential. In a setup where the phase is not controlled externally, we find that the system undergoes a first-order topological phase transition when the Zeeman field is varied. At the transition, the phase difference in the ground state changes abruptly from a value close to zero, at which the system is trivial, to a value close to π, at which the system is topological. The critical current through the junction exhibits a sharp minimum at the critical Zeeman field and is therefore a natural diagnostic of the transition. We point out that in the presence of a symmetry under a mirror reflection followed by time reversal, the system belongs to a higher symmetry class, and the phase diagram as a function of the phase difference and the Zeeman field becomes richer.
url http://doi.org/10.1103/PhysRevX.7.021032
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AT adystern topologicalsuperconductivityinaplanarjosephsonjunction
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