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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...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2017
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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. |
format | Online Article Text |
id | pubmed-5474691 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
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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