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dc.contributor.authorBoyack, Rufusen_US
dc.contributor.authorWu, Chien-Teen_US
dc.contributor.authorAnderson, Brandon M.en_US
dc.contributor.authorLevin, K.en_US
dc.date.accessioned2019-04-03T06:41:50Z-
dc.date.available2019-04-03T06:41:50Z-
dc.date.issued2017-06-02en_US
dc.identifier.issn2469-9950en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.95.214501en_US
dc.identifier.urihttp://hdl.handle.net/11536/146120-
dc.description.abstractIn this paper we demonstrate the necessity of including the generally omitted collective-mode contributions in calculations of the Meissner effect for nonuniform superconductors. We consider superconducting pairing with nonzero center-of-mass momentum, as is possibly relevant to high transition temperature cuprates, cold atoms, and color superconductors in quantum chromodynamics. For the concrete example of the Fulde-Ferrell phase we present a quantitative calculation of the superfluid density, showing not only that the collective-mode contributions are appreciable but also that they derive from the amplitude mode of the order parameter. This latter mode is generally viewed as being invisible in conventional superconductors. However, our analysis shows that it is extremely important in pair-density-wave-type superconductors, where it destroys stable superfluidity well before the mean-field order parameter vanishes.en_US
dc.language.isoen_USen_US
dc.titleCollective mode contributions to the Meissner effect: Fulde-Ferrell and pair-density wave superfluidsen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.95.214501en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume95en_US
dc.citation.issue21en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000411567500001en_US
dc.citation.woscount0en_US
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