Majorana Zero Modes in Graphene

A clear demonstration of topological superconductivity (TS) and Majorana zero modes remains one of the major pending goals in the field of topological materials. One common strategy to generate TS is through the coupling of an s-wave superconductor to a helical half-metallic system. Numerous proposa...

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Main Authors: P. San-Jose, J. L. Lado, R. Aguado, F. Guinea, J. Fernández-Rossier
Format: Article
Language:English
Published: American Physical Society 2015-12-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.5.041042
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spelling doaj-0fb8592eca2742deb6219c02038ece5a2020-11-25T00:29:15ZengAmerican Physical SocietyPhysical Review X2160-33082015-12-015404104210.1103/PhysRevX.5.041042Majorana Zero Modes in GrapheneP. San-JoseJ. L. LadoR. AguadoF. GuineaJ. Fernández-RossierA clear demonstration of topological superconductivity (TS) and Majorana zero modes remains one of the major pending goals in the field of topological materials. One common strategy to generate TS is through the coupling of an s-wave superconductor to a helical half-metallic system. Numerous proposals for the latter have been put forward in the literature, most of them based on semiconductors or topological insulators with strong spin-orbit coupling. Here, we demonstrate an alternative approach for the creation of TS in graphene-superconductor junctions without the need for spin-orbit coupling. Our prediction stems from the helicity of graphene’s zero-Landau-level edge states in the presence of interactions and from the possibility, experimentally demonstrated, of tuning their magnetic properties with in-plane magnetic fields. We show how canted antiferromagnetic ordering in the graphene bulk close to neutrality induces TS along the junction and gives rise to isolated, topologically protected Majorana bound states at either end. We also discuss possible strategies to detect their presence in graphene Josephson junctions through Fraunhofer pattern anomalies and Andreev spectroscopy. The latter, in particular, exhibits strong unambiguous signatures of the presence of the Majorana states in the form of universal zero-bias anomalies. Remarkable progress has recently been reported in the fabrication of the proposed type of junctions, which offers a promising outlook for Majorana physics in graphene systems.http://doi.org/10.1103/PhysRevX.5.041042
collection DOAJ
language English
format Article
sources DOAJ
author P. San-Jose
J. L. Lado
R. Aguado
F. Guinea
J. Fernández-Rossier
spellingShingle P. San-Jose
J. L. Lado
R. Aguado
F. Guinea
J. Fernández-Rossier
Majorana Zero Modes in Graphene
Physical Review X
author_facet P. San-Jose
J. L. Lado
R. Aguado
F. Guinea
J. Fernández-Rossier
author_sort P. San-Jose
title Majorana Zero Modes in Graphene
title_short Majorana Zero Modes in Graphene
title_full Majorana Zero Modes in Graphene
title_fullStr Majorana Zero Modes in Graphene
title_full_unstemmed Majorana Zero Modes in Graphene
title_sort majorana zero modes in graphene
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2015-12-01
description A clear demonstration of topological superconductivity (TS) and Majorana zero modes remains one of the major pending goals in the field of topological materials. One common strategy to generate TS is through the coupling of an s-wave superconductor to a helical half-metallic system. Numerous proposals for the latter have been put forward in the literature, most of them based on semiconductors or topological insulators with strong spin-orbit coupling. Here, we demonstrate an alternative approach for the creation of TS in graphene-superconductor junctions without the need for spin-orbit coupling. Our prediction stems from the helicity of graphene’s zero-Landau-level edge states in the presence of interactions and from the possibility, experimentally demonstrated, of tuning their magnetic properties with in-plane magnetic fields. We show how canted antiferromagnetic ordering in the graphene bulk close to neutrality induces TS along the junction and gives rise to isolated, topologically protected Majorana bound states at either end. We also discuss possible strategies to detect their presence in graphene Josephson junctions through Fraunhofer pattern anomalies and Andreev spectroscopy. The latter, in particular, exhibits strong unambiguous signatures of the presence of the Majorana states in the form of universal zero-bias anomalies. Remarkable progress has recently been reported in the fabrication of the proposed type of junctions, which offers a promising outlook for Majorana physics in graphene systems.
url http://doi.org/10.1103/PhysRevX.5.041042
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