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dc.contributor.authorLin, JYen_US
dc.contributor.authorLin, PHen_US
dc.contributor.authorHo, PLen_US
dc.contributor.authorHuang, HLen_US
dc.contributor.authorZhang, YLen_US
dc.contributor.authorYu, RCen_US
dc.contributor.authorJin, CQen_US
dc.contributor.authorYang, HDen_US
dc.date.accessioned2014-12-08T15:41:53Z-
dc.date.available2014-12-08T15:41:53Z-
dc.date.issued2002-10-01en_US
dc.identifier.issn0896-1107en_US
dc.identifier.urihttp://hdl.handle.net/11536/28485-
dc.description.abstractH-c2 of MgCNi3 has been determined from the specific heat C and resistivity rho measurements in the same sample. The results from rho are nearly identical with those determined from the anomaly in C. Furthermore, utilizing the relation gamma(H) proportional to H and the value of dgamma/dH, the obtained value of H-c2 is the same as that by the WHH model, if the spin paramagnetic effect and the spin-orbit interaction are taken into account. The results of this comparison have strong implications on the order parameter of MgCNi3.en_US
dc.language.isoen_USen_US
dc.subjectMgCNi3en_US
dc.subjectH-c2en_US
dc.subjectspecific heaten_US
dc.subjectorder parameteren_US
dc.subjectmixed stateen_US
dc.titleH-c2 of MgCNi3 determined from the specific heat and resistivity measurementsen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.journalJOURNAL OF SUPERCONDUCTIVITYen_US
dc.citation.volume15en_US
dc.citation.issue5en_US
dc.citation.spage485en_US
dc.citation.epage488en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000179847600036-
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