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dc.contributor.authorWei, JCen_US
dc.contributor.authorYang, TJen_US
dc.date.accessioned2014-12-08T15:02:16Z-
dc.date.available2014-12-08T15:02:16Z-
dc.date.issued1996-11-01en_US
dc.identifier.issn0021-4922en_US
dc.identifier.urihttp://hdl.handle.net/11536/965-
dc.description.abstractThe current distribution due to a single vortex in a superconducting film of finite thickness is calculated, based on the London model. At large distances from the vortex core, the current density on the surface of the superconductor was found to follow the 1/r(2) law which has a simple expression, J(s)(r, 0) approximate to phi(0)[coth(d/lambda) + csch (d/lambda)]/2 pi mu(0) lambda r(2). We also find that the interaction energy between two vortices has the form, U-int(r/(12)) phi(0)(2)[H-0(r(12)/lambda') - Y-0(r(12)/lambda l)], when the film is not too thick and at large distances between two vortices. This potential differs from Pearl's result by the new effective penetration depth lambda' = 2 lambda coth (d/lambda).en_US
dc.language.isoen_USen_US
dc.subjectsuperconducting filmen_US
dc.subjectLondon modelen_US
dc.subjecteffective penetration depthen_US
dc.titleCurrent distribution and vortex-vortex interaction in a superconducting film of finite thicknessen_US
dc.typeArticleen_US
dc.identifier.journalJAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS SHORT NOTES & REVIEW PAPERSen_US
dc.citation.volume35en_US
dc.citation.issue11en_US
dc.citation.spage5696en_US
dc.citation.epage5700en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:A1996VV24100023-
dc.citation.woscount15-
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