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Ginzburg-Landau theory of superconducting surfaces under the influence of electric fields

dc.citation.epage0en_US
dc.citation.issue5en_US
dc.citation.spage0en_US
dc.citation.volume73en_US
dc.citation.woscount11en_US
dc.contributor.authorLipavsky, Pen_US
dc.contributor.authorMorawetz, Ken_US
dc.contributor.authorKolacek, Jen_US
dc.contributor.authorYang, TJen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.date.accessioned2019-04-03T06:44:59Z
dc.date.available2019-04-03T06:44:59Z
dc.date.issued2006-02-01en_US
dc.description.abstractA boundary condition for the Ginzburg-Landau wave function at surfaces biased by a strong electric field is derived within the de Gennes approach. This condition provides a simple theory of the field effect on the critical temperature of superconducting layers.en_US
dc.identifier.doi10.1103/PhysRevB.73.052505en_US
dc.identifier.issn1098-0121en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.73.052505en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/12644
dc.identifier.wosnumberWOS:000235668300021en_US
dc.language.isoen_USen_US
dc.titleGinzburg-Landau theory of superconducting surfaces under the influence of electric fieldsen_US
dc.typeArticleen_US

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