Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/15077
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dc.contributor.authorUdomsamuthirun P.
dc.contributor.authorKumvongsa C.
dc.contributor.authorBurakorn A.
dc.contributor.authorChangkanarth P.
dc.contributor.authorYoksan S.
dc.date.accessioned2021-04-05T04:32:30Z-
dc.date.available2021-04-05T04:32:30Z-
dc.date.issued2005
dc.identifier.issn9214534
dc.identifier.other2-s2.0-24144433864
dc.identifier.urihttps://ir.swu.ac.th/jspui/handle/123456789/15077-
dc.identifier.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-24144433864&doi=10.1016%2fj.physc.2005.07.001&partnerID=40&md5=5f8d39b834037c45a2b9a8d3f207fa9c
dc.description.abstractThe exact formula of Tc's equation and the isotope effect exponent of two-band s-wave superconductors in weak-coupling limit are derived by considering the influence of two kinds of density of state: constant and van Hove singularity. The paring interaction in each band consisted of two parts: the electron-phonon interaction and non-electron-phonon interaction are included in our model. We find that the interband interaction of electron-phonon show more effect on isotope exponent than the intraband interaction and the isotope effect exponent with constant density of state can fit to experimental data, MgB2 and high-Tc superconductor, better than van Hove singularity density of state. © 2005 Elsevier B.V. All rights reserved.
dc.subjectCurrent density
dc.subjectElectrons
dc.subjectPhonons
dc.subjectDensity of state
dc.subjectIsotope effect exponent
dc.subjectTwo-band superconductors
dc.subjectWeak coupling
dc.subjectSuperconducting materials
dc.titleEffect of density of state on isotope effect exponent of two-band superconductors
dc.typeArticle
dc.rights.holderScopus
dc.identifier.bibliograpycitationPhysica C: Superconductivity and its Applications. Vol 425, (2005), p.149-154
dc.identifier.doi10.1016/j.physc.2005.07.001
Appears in Collections:Scopus 1983-2021

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