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dc.contributor.authorLi, D.en_US
dc.contributor.authorLin, P. J.en_US
dc.contributor.authorRosenstein, B.en_US
dc.date.accessioned2014-12-08T15:42:33Z-
dc.date.available2014-12-08T15:42:33Z-
dc.date.issued2008-09-15en_US
dc.identifier.issn0921-4534en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.physc.2008.05.266en_US
dc.identifier.urihttp://hdl.handle.net/11536/28887-
dc.description.abstractPhase diagram of both high temperature superconductors and low temperature superconductors are studied within the Ginzburg-Landau approach. Due to enhanced thermal fluctuation strength, disorder effects are relatively small in high T-c superconductors and consequently can be studied analytically. The vortex glass transition line is different and well separated from both the melting line and from the so-called second peak lines. On contrary, in low temperature superconductors, the disorder effect is dominant, as the thermal fluctuation strength is very small. Peak effect appears due to cross over of the collective pinning region to stronger pinning region. The location of the peak effect is obtained. The disorder and thermal fluctuation effects on structure phase transition are also studied. (C) 2008 Elsevier B.V. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectvortex matteren_US
dc.subjectglass phaseen_US
dc.subjectmeltingen_US
dc.subjectpeak effecten_US
dc.titleMagnetic phase diagram of type-II superconductors: From high T-c to low T-c superconductorsen_US
dc.typeArticle; Proceedings Paperen_US
dc.identifier.doi10.1016/j.physc.2008.05.266en_US
dc.identifier.journalPHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONSen_US
dc.citation.volume468en_US
dc.citation.issue15-20en_US
dc.citation.spage1245en_US
dc.citation.epage1248en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000259712900041-
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