Transitions of I- and II-order in magnetic field for superconducting cylinder from self-consistent solution of Ginzburg-Landau equations

dc.creatorZharkov, G. F.
dc.date2000-10-02
dc.date2000-10-04
dc.date.accessioned2026-07-07T02:38:54Z
dc.date.available2026-07-07T02:38:54Z
dc.descriptionBasing on self-consistent solution of non-linear GL-equations, the phase boundary is found, which divides the regions of I- and II-order phase transitions of a superconducting cylinder in magnetic field to normal state. This boundary is a complicated function of the parameters (m,R,kappa) (m is the vorticity, R is the cylinder radius, kappa is the GL-parameter), which does not coincide with the simple phase boundary kappa=1/\sqrt{2}, dividing the regions of I- and II-order phase transitions in infinite (open) superconducting systems.
dc.description5 pages, 5 figures, RevTex (missing Figs. are added)
dc.identifierhttps://arxiv.org/abs/cond-mat/0010028
dc.identifierhttp://arxiv.org/abs/cond-mat/0010028
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/16856
dc.subjectSuperconductivity
dc.titleTransitions of I- and II-order in magnetic field for superconducting cylinder from self-consistent solution of Ginzburg-Landau equations
dc.typetext

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