Signatures of topological phase transitions in mesoscopic superconducting rings

We investigate Josephson currents in mesoscopic rings with a weak link which are in or near a topological superconducting phase. As a paradigmatic example, we consider the Kitaev model of a spinless p-wave superconductor in one dimension, emphasizing how this model emerges from more realistic settin...

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Main Authors: Falko Pientka, Alessandro Romito, Mathias Duckheim, Yuval Oreg, Felix von Oppen
Format: Article
Language:English
Published: IOP Publishing 2013-01-01
Series:New Journal of Physics
Online Access:https://doi.org/10.1088/1367-2630/15/2/025001
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author Falko Pientka
Alessandro Romito
Mathias Duckheim
Yuval Oreg
Felix von Oppen
author_facet Falko Pientka
Alessandro Romito
Mathias Duckheim
Yuval Oreg
Felix von Oppen
author_sort Falko Pientka
collection DOAJ
description We investigate Josephson currents in mesoscopic rings with a weak link which are in or near a topological superconducting phase. As a paradigmatic example, we consider the Kitaev model of a spinless p-wave superconductor in one dimension, emphasizing how this model emerges from more realistic settings based on semiconductor nanowires. We show that the flux periodicity of the Josephson current provides signatures of the topological phase transition and the emergence of Majorana fermions (MF) situated on both sides of the weak link even when fermion parity is not a good quantum number. In large rings, the MF hybridize only across the weak link. In this case, the Josephson current is h / e periodic in the flux threading the loop when fermion parity is a good quantum number but reverts to the more conventional h /2 e periodicity in the presence of fermion-parity changing relaxation processes. In mesoscopic rings, the MF also hybridize through their overlap in the interior of the superconducting ring. We find that in the topological superconducting phase, this gives rise to an h / e -periodic contribution even when fermion parity is not conserved and that this contribution exhibits a peak near the topological phase transition. This signature of the topological phase transition is robust to the effects of disorder. As a byproduct, we find that close to the topological phase transition, disorder drives the system deeper into the topological phase. This is in stark contrast to the known behavior far from the phase transition, where disorder tends to suppress the topological phase.
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spelling doaj.art-bfcb28aedff1494b948ec8606aba94c12023-08-08T11:04:45ZengIOP PublishingNew Journal of Physics1367-26302013-01-0115202500110.1088/1367-2630/15/2/025001Signatures of topological phase transitions in mesoscopic superconducting ringsFalko Pientka0Alessandro Romito1Mathias Duckheim2Yuval Oreg3Felix von Oppen4Dahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universität Berlin , D-14195 Berlin, GermanyDahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universität Berlin , D-14195 Berlin, GermanyDahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universität Berlin , D-14195 Berlin, GermanyDepartment of Condensed Matter Physics, Weizmann Institute of Science , Rehovot 76100, IsraelDahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universität Berlin , D-14195 Berlin, GermanyWe investigate Josephson currents in mesoscopic rings with a weak link which are in or near a topological superconducting phase. As a paradigmatic example, we consider the Kitaev model of a spinless p-wave superconductor in one dimension, emphasizing how this model emerges from more realistic settings based on semiconductor nanowires. We show that the flux periodicity of the Josephson current provides signatures of the topological phase transition and the emergence of Majorana fermions (MF) situated on both sides of the weak link even when fermion parity is not a good quantum number. In large rings, the MF hybridize only across the weak link. In this case, the Josephson current is h / e periodic in the flux threading the loop when fermion parity is a good quantum number but reverts to the more conventional h /2 e periodicity in the presence of fermion-parity changing relaxation processes. In mesoscopic rings, the MF also hybridize through their overlap in the interior of the superconducting ring. We find that in the topological superconducting phase, this gives rise to an h / e -periodic contribution even when fermion parity is not conserved and that this contribution exhibits a peak near the topological phase transition. This signature of the topological phase transition is robust to the effects of disorder. As a byproduct, we find that close to the topological phase transition, disorder drives the system deeper into the topological phase. This is in stark contrast to the known behavior far from the phase transition, where disorder tends to suppress the topological phase.https://doi.org/10.1088/1367-2630/15/2/025001
spellingShingle Falko Pientka
Alessandro Romito
Mathias Duckheim
Yuval Oreg
Felix von Oppen
Signatures of topological phase transitions in mesoscopic superconducting rings
New Journal of Physics
title Signatures of topological phase transitions in mesoscopic superconducting rings
title_full Signatures of topological phase transitions in mesoscopic superconducting rings
title_fullStr Signatures of topological phase transitions in mesoscopic superconducting rings
title_full_unstemmed Signatures of topological phase transitions in mesoscopic superconducting rings
title_short Signatures of topological phase transitions in mesoscopic superconducting rings
title_sort signatures of topological phase transitions in mesoscopic superconducting rings
url https://doi.org/10.1088/1367-2630/15/2/025001
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