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dc.contributor.authorYang, HDen_US
dc.contributor.authorHong, IPen_US
dc.contributor.authorChatterjee, Sen_US
dc.contributor.authorNachimuthu, Pen_US
dc.contributor.authorChen, JMen_US
dc.contributor.authorLin, JYen_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)00524-4en_US
dc.identifier.urihttp://hdl.handle.net/11536/30151-
dc.description.abstractPrBa2Cu3O7 (Pr123) has attracted much attention due to its non-superconductivity and other anomalies. The very recent reports on superconducting Pr123, instead of putting an end on this issue, virtually stimulate more controversies. One of the proposed explanations for the recently observed superconductivity in Pr123 is that the samples could be Ba-rich Pr123. To investigate this possibility, we have prepared Pr1-xBa2+xCu3O7 With x=0 to 0.3. It is found that resistivity of the samples becomes smaller with increasing x, together with elongation of the c-axis. O K-edge x-ray absorption structure indicates an increase in the carrier concentration with Ba doping. However, carriers are introduced in a peculiar way rather than simply added into CuO2 planes.en_US
dc.language.isoen_USen_US
dc.titleX-ray absorption near-edge structure of Pr1-xBa2+xCu3O7en_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/S0921-4534(00)00524-4en_US
dc.identifier.journalPHYSICA Cen_US
dc.citation.volume341en_US
dc.citation.issueen_US
dc.citation.spage411en_US
dc.citation.epage412en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000165855500141-
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