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dc.contributor.authorChen, Y.-J.en_US
dc.contributor.authorLiu, C.-J.en_US
dc.contributor.authorWang, J.-S.en_US
dc.contributor.authorLin, J.-Y.en_US
dc.contributor.authorSun, C. P.en_US
dc.contributor.authorHuang, S. W.en_US
dc.contributor.authorLee, J. M.en_US
dc.contributor.authorChen, J. M.en_US
dc.contributor.authorLee, J. F.en_US
dc.contributor.authorLiu, D. G.en_US
dc.contributor.authorYang, H. D.en_US
dc.date.accessioned2019-04-03T06:40:53Z-
dc.date.available2019-04-03T06:40:53Z-
dc.date.issued2007-09-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.76.092501en_US
dc.identifier.urihttp://hdl.handle.net/11536/10350-
dc.description.abstractTo shed light on the symmetry of the superconducting order parameter in NaxCoO2 center dot yH(2)O, the Mn doping effects are studied. X-ray absorption spectroscopy verifies that the doped Mn impurities occupy the Co sites and are with a valance close to +4. Impurity scattering by Mn is in the unitary limit that, however, does not lead to strong T-c suppression. This absence of the strong impurity effects on T-c is inconsistent with the simple picture of a sign-changing order parameter. Coexistence of the s-wave superconducting order parameter and the nodal one is proposed to reconcile all the existing experiments and has been implied by the specific heat experiments.en_US
dc.language.isoen_USen_US
dc.titleEffect of Mn impurities on the superconductivity in NaxCoO2 center dot yH(2)Oen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.76.092501en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume76en_US
dc.citation.issue9en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000249786100023en_US
dc.citation.woscount12en_US
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