完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | Chen, JM | en_US |
dc.contributor.author | Chang, SC | en_US |
dc.contributor.author | Liu, RS | en_US |
dc.contributor.author | Lee, JM | en_US |
dc.contributor.author | Park, M | en_US |
dc.contributor.author | Choy, JH | en_US |
dc.date.accessioned | 2014-12-08T15:17:36Z | - |
dc.date.available | 2014-12-08T15:17:36Z | - |
dc.date.issued | 2006-01-01 | en_US |
dc.identifier.issn | 0022-3697 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1016/j.jpcs.2005.10.103 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/12770 | - |
dc.description.abstract | Hole 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.iso | en_US | en_US |
dc.title | Hole states of X-Bi2Sr2CaCu2O8 [X=I, HgI2, and (Py-CH3)(2)HgI4] probed by OK-edge X-ray absorption spectroscopy | en_US |
dc.type | Article; Proceedings Paper | en_US |
dc.identifier.doi | 10.1016/j.jpcs.2005.10.103 | en_US |
dc.identifier.journal | JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS | en_US |
dc.citation.volume | 67 | en_US |
dc.citation.issue | 1-3 | en_US |
dc.citation.spage | 223 | en_US |
dc.citation.epage | 226 | en_US |
dc.contributor.department | 電子物理學系 | zh_TW |
dc.contributor.department | Department of Electrophysics | en_US |
dc.identifier.wosnumber | WOS:000236746600055 | - |
顯示於類別: | 會議論文 |