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dc.contributor.authorRosenstein, B.en_US
dc.contributor.authorShapiro, B. Yaen_US
dc.contributor.authorLi, Dingpingen_US
dc.contributor.authorShapiro, I.en_US
dc.date.accessioned2015-07-21T08:29:27Z-
dc.date.available2015-07-21T08:29:27Z-
dc.date.issued2015-04-01en_US
dc.identifier.issn0022-2291en_US
dc.identifier.urihttp://dx.doi.org/10.1007/s10909-014-1232-3en_US
dc.identifier.urihttp://hdl.handle.net/11536/124493-
dc.description.abstractConventional electron-phonon coupling induces either odd (triplet) or even (singlet) pairing states in a time reversal and inversion invariant Dirac semi-metal. In a certain range of the chemical potential and parameters characterizing the pairing attraction (effective electron-electron coupling constant and the Debye energy ) the energy of the singlet although always lower, prevails by a very slim margin over the triplet. This means that interactions that are small but discriminate between the spin singlet and the spin triplet determine the nature of the superconducting order there. It is shown that in materials close enough to the Dirac point ( ) a moderate exchange constant (below Stoner instability to ferromagnetism) stabilizes the odd pairing superconducting state. The 3D quantum critical point at of transition to the triplet superconductivity governs the physics of the superconductor.en_US
dc.language.isoen_USen_US
dc.subjectDiracen_US
dc.subjectSemi-metalen_US
dc.subjectSuperconductivityen_US
dc.titleExchange Interaction Makes Superconductivity in 3D Dirac Semi-metal Tripleten_US
dc.typeArticleen_US
dc.identifier.doi10.1007/s10909-014-1232-3en_US
dc.identifier.journalJOURNAL OF LOW TEMPERATURE PHYSICSen_US
dc.citation.volume179en_US
dc.citation.issue1-2en_US
dc.citation.spage101en_US
dc.citation.epage107en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000350241200017en_US
dc.citation.woscount0en_US
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