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dc.contributor.authorChen, JMen_US
dc.contributor.authorChang, SCen_US
dc.contributor.authorLiu, RSen_US
dc.contributor.authorLee, JMen_US
dc.contributor.authorPark, Men_US
dc.contributor.authorChoy, JHen_US
dc.date.accessioned2014-12-08T15:17:36Z-
dc.date.available2014-12-08T15:17:36Z-
dc.date.issued2006-01-01en_US
dc.identifier.issn0022-3697en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.jpcs.2005.10.103en_US
dc.identifier.urihttp://hdl.handle.net/11536/12770-
dc.description.abstractHole states of X-Bi2Sr2CaCU2O8[X-Bi2212, X=I, HgI2, and (Py-CH3)(2)-HgI4, Py = pyridinel have been probed by O K-edge X-ray absorption near-edge structure (XANES) spectra. In the O 1s absorption edge of X-Bi2212, the pre-edge peak at similar to 528.3 eV is attributed to transitions into the 0 2p hole states located in the CuO2 planes. The hole concentration in the CuO2 planes of X-Bi2212 increases for X =I and HgI2, but decreases for X= (Py-CH3)(2)HgI4 as coMPared to pristine Bi2212. The variation of CuO2-plane hole concentration of Bi2212 is primarily responsible for the T-c variation upon intercalation. (c) 2005 Elsevier Ltd. All rights reserved.en_US
dc.language.isoen_USen_US
dc.titleHole states of X-Bi2Sr2CaCu2O8 [X=I, HgI2, and (Py-CH3)(2)HgI4] probed by OK-edge X-ray absorption spectroscopyen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/j.jpcs.2005.10.103en_US
dc.identifier.journalJOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDSen_US
dc.citation.volume67en_US
dc.citation.issue1-3en_US
dc.citation.spage223en_US
dc.citation.epage226en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000236746600055-
Appears in Collections:Conferences Paper


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