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...
Main Authors: | , , , , , |
---|---|
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 |
id |
doaj-bd8338b64ff746a9bf3a780fa3da45ac |
---|---|
record_format |
Article |
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 |
work_keys_str_mv |
AT falkopientka topologicalsuperconductivityinaplanarjosephsonjunction AT annakeselman topologicalsuperconductivityinaplanarjosephsonjunction AT erezberg topologicalsuperconductivityinaplanarjosephsonjunction AT amiryacoby topologicalsuperconductivityinaplanarjosephsonjunction AT adystern topologicalsuperconductivityinaplanarjosephsonjunction AT bertrandihalperin topologicalsuperconductivityinaplanarjosephsonjunction |
_version_ |
1716241956285186048 |