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dc.contributor.authorKU, HCen_US
dc.contributor.authorSUN, SJen_US
dc.contributor.authorSHI, JBen_US
dc.date.accessioned2014-12-08T15:05:04Z-
dc.date.available2014-12-08T15:05:04Z-
dc.date.issued1991-12-01en_US
dc.identifier.issn0921-4534en_US
dc.identifier.urihttp://dx.doi.org/10.1016/0921-4534(91)91669-Uen_US
dc.identifier.urihttp://hdl.handle.net/11536/3613-
dc.description.abstractThe structure and superconductivity in the single Cu-O layer bismuth (2021) system can be stabilized also by the doping of Na1+ ions. Contrary to the La-doped Bi2(Sr,La)2CuO6+delta system with T(c) enhancement up to 35 K. T(c) remains around 10 K for the Na-doped Bi2(Sr2-xNax)CuO6+delta system (0.0 less-than-or-equal-to x less-than-or-equal-to 0.4). The variation of T(c) with the Cu-O bond length r(Cu-0) in the Cu-O layer for the Bi family which consists of the systems (Bi,Pb)2Sr2CuO6+delta, Bi2(Sr,Na)2CuO6+delta, Bi2(Sr,La)2CuO6+delta and (Bi,Pb)2(Sr,La)2CuO6+delta indicates an optimum r(Cu-0) value of 1.906-1.913 angstrom with maximum T(c) of 35 K for these Bi(2021) compounds.en_US
dc.language.isoen_USen_US
dc.titleTHE CORRELATION BETWEEN SUPERCONDUCTIVITY AND CU-O BOND LENGTH FOR THE SINGLE CU-O LAYER COMPOUNDS WITH THE BI2SR2CUO6+DELTA-TYPE (2021) STRUCTUREen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/0921-4534(91)91669-Uen_US
dc.identifier.journalPHYSICA Cen_US
dc.citation.volume185en_US
dc.citation.issueen_US
dc.citation.spage891en_US
dc.citation.epage892en_US
dc.contributor.department電控工程研究所zh_TW
dc.contributor.departmentInstitute of Electrical and Control Engineeringen_US
dc.identifier.wosnumberWOS:A1991GW83000080-
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