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dc.contributor.authorLin, JYen_US
dc.contributor.authorChen, SJen_US
dc.contributor.authorChen, SYen_US
dc.contributor.authorChang, CFen_US
dc.contributor.authorYang, HDen_US
dc.contributor.authorTolpygo, SKen_US
dc.contributor.authorGurvitch, Men_US
dc.contributor.authorHsu, YYen_US
dc.contributor.authorKu, HCen_US
dc.date.accessioned2019-04-03T06:39:17Z-
dc.date.available2019-04-03T06:39:17Z-
dc.date.issued1999-03-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.59.6047en_US
dc.identifier.urihttp://hdl.handle.net/11536/31462-
dc.description.abstractWe have studied the impurity effects on the superconducting transition temperature T-c and the upper critical field H-c2 in electron irradiated YBa2Cu3Oy with in-plane oxygen defects and YBa2(Cu1-xZnx)(3)O-y. It is found that the effects of the same type of defects or impurities on T-c are the same regardless of the oxygen contents of the samples. Furthermore, T-c decreases slower in irradiated YBa2Cu3Oy than in YBa2(Cu1-xZnx)(3)O-y. This may be well explained by the model that the scattering due to in-plane oxygen defects is more anisotropic than that due to Zn impurities. The different behavior of the reduced slopes (dH(c2)/dT)(Tc)/(dH(c2)/dT)(Tc0) these two types of samples can also be understood in this context. [S0163-1829(99)08309-5].en_US
dc.language.isoen_USen_US
dc.titleAnisotropic impurity scattering effects on T-c and H-c2 in YBa2Cu3Oxen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.59.6047en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume59en_US
dc.citation.issue9en_US
dc.citation.spage6047en_US
dc.citation.epage6050en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000079254300018en_US
dc.citation.woscount19en_US
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