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dc.contributor.authorLiu, SJen_US
dc.contributor.authorLin, JYen_US
dc.contributor.authorChen, JMen_US
dc.contributor.authorNachimuthu, Pen_US
dc.contributor.authorLuo, CWen_US
dc.contributor.authorWu, KHen_US
dc.contributor.authorJuang, JYen_US
dc.contributor.authorUen, TMen_US
dc.contributor.authorGou, YSen_US
dc.date.accessioned2014-12-08T15:44:40Z-
dc.date.available2014-12-08T15:44:40Z-
dc.date.issued2000-11-01en_US
dc.identifier.issn0921-4534en_US
dc.identifier.urihttp://dx.doi.org/10.1016/S0921-4534(00)00615-8en_US
dc.identifier.urihttp://hdl.handle.net/11536/30152-
dc.description.abstractUnoccupied electronic states of Y1-xPrxCu3O7-y (x = 0 - 1) thin films have been investigated using high-resolution polarization-dependent O K-edge x-ray absorption spectroscopy (XANES). After determining the hole distribution among different oxygen sites of the Pr-doped thin films, we compare the experimental data with the Fehrenbacher and Rice (FR) model and the Liechtenstein and Mazin (LM) model, both of which are based on the hybridization of Pr 4f(z(x2-y2)) and O 2p(pi) orbitals in PrBa2Cu3O7-y. Our experimental results are more consistent with the FR model.en_US
dc.language.isoen_USen_US
dc.titleA comparison between the Fehrenbacher-Rice and the Liechtenstein-Mazin modelsen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/S0921-4534(00)00615-8en_US
dc.identifier.journalPHYSICA Cen_US
dc.citation.volume341en_US
dc.citation.issueen_US
dc.citation.spage615en_US
dc.citation.epage616en_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:000165855500233-
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