Gauge fluctuations and transition temperature for superconducting wires
We consider the Ginzburg-Landau model, confined in an infinitely long rectangular wire of cross-section \(L_{1}\times L_{2}\). Our approach is based on the Gaussian effective potential in the transverse unitarity gauge, which allows to treat gauge contributions in a compact form. The contributions f...
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Published in | arXiv.org |
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Main Authors | , , |
Format | Paper |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
01.08.2005
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Subjects | |
Online Access | Get full text |
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Summary: | We consider the Ginzburg-Landau model, confined in an infinitely long rectangular wire of cross-section \(L_{1}\times L_{2}\). Our approach is based on the Gaussian effective potential in the transverse unitarity gauge, which allows to treat gauge contributions in a compact form. The contributions from the scalar self-interaction and from the gauge fluctuations are clearly identified. Using techniques from dimensional and \(zeta\)-function regularizations, modified by the confinement conditions, we investigate the critical temperature for a wire of transverse dimensions \(L_1\), \(L_2\). Taking the mass term in the form \(m_{0}^2=a(T/T_0 - 1)\), where \(T_0\) is the bulk transition temperature, we obtain equations for the critical temperature as a function of the \(L_{i}'s\) and of \(T_{0}\), and determine the limiting sizes sustaining the transition. A qualitative comparison with some experimental observations is done. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.0508049 |