Josephson current in a graphene SG/ferromagnetic barrier/SG junction

The Josephson current passing through a SG1/FB/SG2graphene junction, where SG and FBare those parts of a graphene layer which are induced into the superconducting state and into the ferromagnetic state, respectively, and where the small thickness of the FBlayer L is studied. The ferromagnetic barrie...

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Main Authors: Bumned Soodchomshom, I. Ming Tang, Rassmidara Hoonsawat
Other Authors: Mahidol University
Format: Article
Published: 2018
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Online Access:https://repository.li.mahidol.ac.th/handle/123456789/19180
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spelling th-mahidol.191802018-07-12T09:52:19Z Josephson current in a graphene SG/ferromagnetic barrier/SG junction Bumned Soodchomshom I. Ming Tang Rassmidara Hoonsawat Mahidol University Energy Engineering Materials Science Physics and Astronomy The Josephson current passing through a SG1/FB/SG2graphene junction, where SG and FBare those parts of a graphene layer which are induced into the superconducting state and into the ferromagnetic state, respectively, and where the small thickness of the FBlayer L is studied. The ferromagnetic barrier strength is taken to be given by χH∼ HL/ℏvF, where H is the strength of the exchange energy and vF∼ 106m/s is the Fermi velocity of quasiparticles. The eigenstates of the relativistic quasiparticles in the graphene are taken to be the solutions of the Dirac Bogoliubov-de Gennes equations. It is found that the energy levels of the Andreev bound states for the Weyl-Dirac particles in the SG1/FB/SG2junction are independent of the direction of the spins and that they depend on the strength of ferromagnetic barrier potential. The critical supercurrent is seen to vary in an oscillatory (periodic) manner as χHis varied. The oscillatory behavior of the critical supercurrent carried by the Cooper pairs formed by massless the Weyl-Dirac particles is different from the behavior of the supercurrent carried by the Cooper pairs formed by non-relativistic particles in a conventional SC/FI/SC (FI being a ferromagnetic insulator) junction. In those types of junctions, the supercurrent does not exhibit a similar oscillatory dependence. © 2008 Elsevier B.V. All rights reserved. 2018-07-12T02:25:40Z 2018-07-12T02:25:40Z 2008-12-15 Article Physica C: Superconductivity and its Applications. Vol.468, No.24 (2008), 2361-2365 10.1016/j.physc.2008.08.012 09214534 2-s2.0-56149098862 https://repository.li.mahidol.ac.th/handle/123456789/19180 Mahidol University SCOPUS https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=56149098862&origin=inward
institution Mahidol University
building Mahidol University Library
continent Asia
country Thailand
Thailand
content_provider Mahidol University Library
collection Mahidol University Institutional Repository
topic Energy
Engineering
Materials Science
Physics and Astronomy
spellingShingle Energy
Engineering
Materials Science
Physics and Astronomy
Bumned Soodchomshom
I. Ming Tang
Rassmidara Hoonsawat
Josephson current in a graphene SG/ferromagnetic barrier/SG junction
description The Josephson current passing through a SG1/FB/SG2graphene junction, where SG and FBare those parts of a graphene layer which are induced into the superconducting state and into the ferromagnetic state, respectively, and where the small thickness of the FBlayer L is studied. The ferromagnetic barrier strength is taken to be given by χH∼ HL/ℏvF, where H is the strength of the exchange energy and vF∼ 106m/s is the Fermi velocity of quasiparticles. The eigenstates of the relativistic quasiparticles in the graphene are taken to be the solutions of the Dirac Bogoliubov-de Gennes equations. It is found that the energy levels of the Andreev bound states for the Weyl-Dirac particles in the SG1/FB/SG2junction are independent of the direction of the spins and that they depend on the strength of ferromagnetic barrier potential. The critical supercurrent is seen to vary in an oscillatory (periodic) manner as χHis varied. The oscillatory behavior of the critical supercurrent carried by the Cooper pairs formed by massless the Weyl-Dirac particles is different from the behavior of the supercurrent carried by the Cooper pairs formed by non-relativistic particles in a conventional SC/FI/SC (FI being a ferromagnetic insulator) junction. In those types of junctions, the supercurrent does not exhibit a similar oscillatory dependence. © 2008 Elsevier B.V. All rights reserved.
author2 Mahidol University
author_facet Mahidol University
Bumned Soodchomshom
I. Ming Tang
Rassmidara Hoonsawat
format Article
author Bumned Soodchomshom
I. Ming Tang
Rassmidara Hoonsawat
author_sort Bumned Soodchomshom
title Josephson current in a graphene SG/ferromagnetic barrier/SG junction
title_short Josephson current in a graphene SG/ferromagnetic barrier/SG junction
title_full Josephson current in a graphene SG/ferromagnetic barrier/SG junction
title_fullStr Josephson current in a graphene SG/ferromagnetic barrier/SG junction
title_full_unstemmed Josephson current in a graphene SG/ferromagnetic barrier/SG junction
title_sort josephson current in a graphene sg/ferromagnetic barrier/sg junction
publishDate 2018
url https://repository.li.mahidol.ac.th/handle/123456789/19180
_version_ 1763498082914271232