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dc.contributor.authorLin, J.-Y.en_US
dc.contributor.authorChen, Y.-J.en_US
dc.contributor.authorLiu, C.-J.en_US
dc.contributor.authorWang, J.-S.en_US
dc.contributor.authorSun, C. P.en_US
dc.contributor.authorYang, H. D.en_US
dc.date.accessioned2014-12-08T15:05:37Z-
dc.date.available2014-12-08T15:05:37Z-
dc.date.issued2007-09-01en_US
dc.identifier.issn0921-4534en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.physc.2007.03.285en_US
dc.identifier.urihttp://hdl.handle.net/11536/4163-
dc.description.abstractC(T) of NaxCo0.99Mn0.01O2 center dot yH(2)O is studied to reveal more details on the nature of the doped Mn ions and the T-c suppression. The extra specific heat contribution in NaxCo0.99Mn0.01O2 center dot yH(2)O manifests the induced local magnetic moment due to Mn doping. The absence of the superconducting transition peak in C(T) of NaxCo0.99Mn0.01O2 center dot yH(2)O suggests a reduced superconducting volume fraction. (C) 2007 Elsevier B.V. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectcobaltateen_US
dc.subjectspecific heaten_US
dc.subjectmagnetic momenten_US
dc.subjectimpurity effecten_US
dc.subjectsuperconducting order parameteren_US
dc.titleSpecific heat of Mn-doped NaxCoO2 center dot yH(2)Oen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/j.physc.2007.03.285en_US
dc.identifier.journalPHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONSen_US
dc.citation.volume460en_US
dc.citation.issueen_US
dc.citation.spage475en_US
dc.citation.epage476en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000249870500152-
Appears in Collections:Conferences Paper


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