Publication:
The study on penetration depth of anisotropic two-band superconductors by Ginzburg–Landau approach

dc.contributor.authorTongkhonburi P.
dc.contributor.authorUdomsamuthirun P.
dc.date.accessioned2021-04-05T03:03:10Z
dc.date.available2021-04-05T03:03:10Z
dc.date.issued2019
dc.date.issuedBE2562
dc.description.abstractThe penetration depth of anisotropic two-band superconductors have been studied by Ginzburg–Landau approach. The anisotropic Fermi surfaces and order parameters with the spherical ellipse or pancake Fermi shape are used for derive penetration depth equation. The numerical calculation of pancake-pancake and pancake-ellipse Fermi sphere shape are fits well with the experiment data of MgB 2 and CaAlSi superconductor, consequently. Our model should be the way to increase understanding in the microscopic mechanism of occurrence of the penetration depth in superconductivity state of these material. © 2019
dc.format.mimetypeapplication/pdf
dc.identifier.citationPhysica C: Superconductivity and its Applications. Vol 561, (2019), p.45-48
dc.identifier.doi10.1016/j.physc.2019.03.014
dc.identifier.issn9214534
dc.identifier.other2-s2.0-85063204759
dc.identifier.urihttps://hdl.handle.net/20.500.14740/5303
dc.rights.holderมหาวิทยาลัยศรีนครินทรวิโรฒ
dc.subject.otherAluminum compounds
dc.subject.otherAnisotropy
dc.subject.otherBoron compounds
dc.subject.otherCalcium compounds
dc.subject.otherMagnesium compounds
dc.subject.otherShear waves
dc.subject.otherSilicon compounds
dc.subject.otherSuperconducting materials
dc.subject.other74.20. Fg
dc.subject.other74.70. Ad
dc.subject.otherAnisotropic superconductors
dc.subject.otherS-waves
dc.subject.otherTwo-band superconductors
dc.subject.otherPenetration depth (superconductivity)
dc.titleThe study on penetration depth of anisotropic two-band superconductors by Ginzburg–Landau approach
dc.typeArticle
dspace.entity.typePublication
swu.datasource.scopushttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85063204759&doi=10.1016%2fj.physc.2019.03.014&partnerID=40&md5=6185b5475038c81a009944774c13b84b

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