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dc.contributor.authorChen, Y-Jen_US
dc.contributor.authorLin, P. J.en_US
dc.contributor.authorWu, K. H.en_US
dc.contributor.authorRosenstein, B.en_US
dc.contributor.authorLuo, C. W.en_US
dc.contributor.authorJuang, J. Y.en_US
dc.contributor.authorLin, J-Yen_US
dc.date.accessioned2014-12-08T15:32:22Z-
dc.date.available2014-12-08T15:32:22Z-
dc.date.issued2013-10-01en_US
dc.identifier.issn0953-2048en_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-2048/26/10/105029en_US
dc.identifier.urihttp://hdl.handle.net/11536/22729-
dc.description.abstractThe comprehensive rho(T) measurements and the consequent resistivity curvature mapping (RCM) on Y0.7Ca0.3Ba2Cu3O7-delta thin films (doping levels p = 0.08-0.21) elucidate a phase diagram for the whole doping range. This phase diagram further strengthens a view that the 'normal' phase in hole-doped cuprates should be divided into a strong superconducting (SC) fluctuation phase and the 'real' normal phase in which there is no significant influence of SC. The temperature of superconducting fluctuations T-f as a function of p was calculated using the Ginzburg-Landau model for layered superconductors. Comparisons between T-f and the Nernst temperature establish the origin of the Nernst effect as SC fluctuations. Some of the details in rho(T) cannot be fully understood by the existing models and call for a more sophisticated theory of carrier dynamics in cuprates.en_US
dc.language.isoen_USen_US
dc.titleSuperconducting fluctuations and the Nernst effect in high-T-c superconductorsen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/0953-2048/26/10/105029en_US
dc.identifier.journalSUPERCONDUCTOR SCIENCE & TECHNOLOGYen_US
dc.citation.volume26en_US
dc.citation.issue10en_US
dc.citation.epageen_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:000324431000031-
dc.citation.woscount2-
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