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Current-Phase Relation of Ballistic Graphene Josephson Junctions

[Image: see text] The current-phase relation (CPR) of a Josephson junction (JJ) determines how the supercurrent evolves with the superconducting phase difference across the junction. Knowledge of the CPR is essential in order to understand the response of a JJ to various external parameters. Despite...

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Autores principales: Nanda, G., Aguilera-Servin, J. L., Rakyta, P., Kormányos, A., Kleiner, R., Koelle, D., Watanabe, K., Taniguchi, T., Vandersypen, L. M. K., Goswami, S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2017
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5474691/
https://www.ncbi.nlm.nih.gov/pubmed/28474892
http://dx.doi.org/10.1021/acs.nanolett.7b00097
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author Nanda, G.
Aguilera-Servin, J. L.
Rakyta, P.
Kormányos, A.
Kleiner, R.
Koelle, D.
Watanabe, K.
Taniguchi, T.
Vandersypen, L. M. K.
Goswami, S.
author_facet Nanda, G.
Aguilera-Servin, J. L.
Rakyta, P.
Kormányos, A.
Kleiner, R.
Koelle, D.
Watanabe, K.
Taniguchi, T.
Vandersypen, L. M. K.
Goswami, S.
author_sort Nanda, G.
collection PubMed
description [Image: see text] The current-phase relation (CPR) of a Josephson junction (JJ) determines how the supercurrent evolves with the superconducting phase difference across the junction. Knowledge of the CPR is essential in order to understand the response of a JJ to various external parameters. Despite the rising interest in ultraclean encapsulated graphene JJs, the CPR of such junctions remains unknown. Here, we use a fully gate-tunable graphene superconducting quantum intereference device (SQUID) to determine the CPR of ballistic graphene JJs. Each of the two JJs in the SQUID is made with graphene encapsulated in hexagonal boron nitride. By independently controlling the critical current of the JJs, we can operate the SQUID either in a symmetric or asymmetric configuration. The highly asymmetric SQUID allows us to phase-bias one of the JJs and thereby directly obtain its CPR. The CPR is found to be skewed, deviating significantly from a sinusoidal form. The skewness can be tuned with the gate voltage and oscillates in antiphase with Fabry-Pérot resistance oscillations of the ballistic graphene cavity. We compare our experiments with tight-binding calculations that include realistic graphene–superconductor interfaces and find a good qualitative agreement.
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spelling pubmed-54746912017-06-21 Current-Phase Relation of Ballistic Graphene Josephson Junctions Nanda, G. Aguilera-Servin, J. L. Rakyta, P. Kormányos, A. Kleiner, R. Koelle, D. Watanabe, K. Taniguchi, T. Vandersypen, L. M. K. Goswami, S. Nano Lett [Image: see text] The current-phase relation (CPR) of a Josephson junction (JJ) determines how the supercurrent evolves with the superconducting phase difference across the junction. Knowledge of the CPR is essential in order to understand the response of a JJ to various external parameters. Despite the rising interest in ultraclean encapsulated graphene JJs, the CPR of such junctions remains unknown. Here, we use a fully gate-tunable graphene superconducting quantum intereference device (SQUID) to determine the CPR of ballistic graphene JJs. Each of the two JJs in the SQUID is made with graphene encapsulated in hexagonal boron nitride. By independently controlling the critical current of the JJs, we can operate the SQUID either in a symmetric or asymmetric configuration. The highly asymmetric SQUID allows us to phase-bias one of the JJs and thereby directly obtain its CPR. The CPR is found to be skewed, deviating significantly from a sinusoidal form. The skewness can be tuned with the gate voltage and oscillates in antiphase with Fabry-Pérot resistance oscillations of the ballistic graphene cavity. We compare our experiments with tight-binding calculations that include realistic graphene–superconductor interfaces and find a good qualitative agreement. American Chemical Society 2017-05-05 2017-06-14 /pmc/articles/PMC5474691/ /pubmed/28474892 http://dx.doi.org/10.1021/acs.nanolett.7b00097 Text en Copyright © 2017 American Chemical Society This is an open access article published under a Creative Commons Non-Commercial No Derivative Works (CC-BY-NC-ND) Attribution License (http://pubs.acs.org/page/policy/authorchoice_ccbyncnd_termsofuse.html) , which permits copying and redistribution of the article, and creation of adaptations, all for non-commercial purposes.
spellingShingle Nanda, G.
Aguilera-Servin, J. L.
Rakyta, P.
Kormányos, A.
Kleiner, R.
Koelle, D.
Watanabe, K.
Taniguchi, T.
Vandersypen, L. M. K.
Goswami, S.
Current-Phase Relation of Ballistic Graphene Josephson Junctions
title Current-Phase Relation of Ballistic Graphene Josephson Junctions
title_full Current-Phase Relation of Ballistic Graphene Josephson Junctions
title_fullStr Current-Phase Relation of Ballistic Graphene Josephson Junctions
title_full_unstemmed Current-Phase Relation of Ballistic Graphene Josephson Junctions
title_short Current-Phase Relation of Ballistic Graphene Josephson Junctions
title_sort current-phase relation of ballistic graphene josephson junctions
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5474691/
https://www.ncbi.nlm.nih.gov/pubmed/28474892
http://dx.doi.org/10.1021/acs.nanolett.7b00097
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