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Two-component Ginzburg–Landau theory of superconducting surfaces in transverse electric field
A boundary condition for the Ginzburg–Landau wave function of a two-component superconductor at surfaces biased by a strong transverse electric field is derived within the de Gennes approach. This boundary condition depends on two correlation lengths of order parameters. A small correlation length l...
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Published in: | Journal of non-crystalline solids 2010-08, Vol.356 (37), p.2056-2058 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | A boundary condition for the Ginzburg–Landau wave function of a two-component superconductor at surfaces biased by a strong transverse electric field is derived within the de Gennes approach. This boundary condition depends on two correlation lengths of order parameters. A small correlation length leads to the oscillations of the shift of the critical temperature of superconducting layers in the transverse electric field on layer width
L. The superconducting temperature
T
c oscillates with the layer width also in the absence of the electric field in the two-band model. A simple theory of the field effect on the superconducting temperature of layers is developed. |
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ISSN: | 0022-3093 1873-4812 |
DOI: | 10.1016/j.jnoncrysol.2010.05.039 |