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Supercooled vortex liquid and superheated vortex solid in type II superconductors

dc.citation.epage611en_US
dc.citation.issue3en_US
dc.citation.spage598en_US
dc.citation.volume43en_US
dc.contributor.authorChen, Len_US
dc.contributor.authorLi, DPen_US
dc.contributor.authorRosenstein, Ben_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.date.accessioned2014-12-08T15:18:58Z
dc.date.available2014-12-08T15:18:58Z
dc.date.issued2005-06-01en_US
dc.description.abstractmetastable homogeneous state exists down to zero temperature in systems of repelling objects. Zero "fluctuation temperature" liquid state therefore serves as a (pseudo) "fixed point" controlling the properties of vortex liquid below and even around melting point. There exists Madelung constant for the liquid in the limit of zero temperature which is higher than that of the solid by an amount approximately equal to the latent heat of melting. On the other hand, the superheated solid exists until the spinodal line. This picture is supported by an exactly solvable large N Ginzburg - Landau model in magnetic field and it is confirmed by the recent experiment.en_US
dc.identifier.issn0577-9073en_US
dc.identifier.journalCHINESE JOURNAL OF PHYSICSen_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/13624
dc.identifier.wosnumberWOS:000230159800015
dc.language.isoen_USen_US
dc.titleSupercooled vortex liquid and superheated vortex solid in type II superconductorsen_US
dc.typeArticle; Proceedings Paperen_US

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