完整後設資料紀錄
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dc.contributor.authorLee, C. C.en_US
dc.contributor.authorLee, W. L.en_US
dc.contributor.authorLin, J. -Y.en_US
dc.contributor.authorTsuei, C. C.en_US
dc.contributor.authorLin, J. G.en_US
dc.contributor.authorChou, F. C.en_US
dc.date.accessioned2014-12-08T15:11:55Z-
dc.date.available2014-12-08T15:11:55Z-
dc.date.issued2011-03-14en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.83.104503en_US
dc.identifier.urihttp://hdl.handle.net/11536/9149-
dc.description.abstractbeta-pyrochore KOs(2)O(6), which shows superconductivity below similar to 9.7 K, has been converted into K(x)Os(2)O(6) (x less than or similar to 2/3-1/2) electrochemically to show spin-glass-like behavior below similar to 6.1 K. A room-temperature sample surface potential versus charge transfer scan indicates that there are at least two two-phase regions for x between 1 and 0.5. A rattling model of superconductivity for the title compound has been examined using electrochemical potassium de-intercalation. The significant reduction of superconducting volume fraction due to minor potassium reduction suggests the importance of defect and phase coherence in the rattling model. Magnetic susceptibility, resistivity, and specific heat measurement results have been compared between the superconducting and spin-glass-like samples.en_US
dc.language.isoen_USen_US
dc.titleSuperconducting to spin-glass state transformation in beta-pyrochlore K(x)Os(2)O(6)en_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.83.104503en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume83en_US
dc.citation.issue10en_US
dc.citation.spageen_US
dc.citation.epageen_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
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