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dc.contributor.authorLo, Shun-Tsungen_US
dc.contributor.authorLin, Shih-Weien_US
dc.contributor.authorWang, Yi-Tingen_US
dc.contributor.authorLin, Sheng-Dien_US
dc.contributor.authorLiang, C. -T.en_US
dc.date.accessioned2019-04-03T06:43:10Z-
dc.date.available2019-04-03T06:43:10Z-
dc.date.issued2014-06-25en_US
dc.identifier.issn2045-2322en_US
dc.identifier.urihttp://dx.doi.org/10.1038/srep05438en_US
dc.identifier.urihttp://hdl.handle.net/11536/24636-
dc.description.abstractSuperconductivity and spin-orbit (SO) interaction have been two separate emerging fields until very recently that the correlation between them seemed to be observed. However, previous experiments concerning SO coupling are performed far beyond the superconducting state and thus a direct demonstration of how SO coupling affects superconductivity remains elusive. Here we investigate the SO coupling in the critical region of superconducting transition on Al nanofilms, in which the strength of disorder and spin relaxation by SO coupling are changed by varying the film thickness. At temperatures T sufficiently above the superconducting critical temperature T-c, clear signature of SO coupling reveals itself in showing a magneto-resistivity peak. When T < T-c, the resistivity peak can still be observed; however, its line-shape is now affected by the onset of the quasi two-dimensional superconductivity. By studying such magneto-resistivity peaks under different strength of spin relaxation, we highlight the important effects of SO interaction on superconductivity.en_US
dc.language.isoen_USen_US
dc.titleSpin-orbit-coupled superconductivityen_US
dc.typeArticleen_US
dc.identifier.doi10.1038/srep05438en_US
dc.identifier.journalSCIENTIFIC REPORTSen_US
dc.citation.volume4en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子工程學系及電子研究所zh_TW
dc.contributor.departmentDepartment of Electronics Engineering and Institute of Electronicsen_US
dc.identifier.wosnumberWOS:000337890600012en_US
dc.citation.woscount8en_US
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