Gauge fluctuations and transition temperature for superconducting wires

preprint2005arXivOpen access

Abstract

We consider the Ginzburg-Landau model, confined in an infinitely long rectangular wire of cross-section L1×L2L_{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 zetazeta-function regularizations, modified by the confinement conditions, we investigate the critical temperature for a wire of transverse dimensions L1L_1, L2L_2. Taking the mass term in the form m02=a(T/T0−1)m_{0}^2=a(T/T_0 - 1), where T0T_0 is the bulk transition temperature, we obtain equations for the critical temperature as a function of the Li′sL_{i}'s and of T0T_{0}, and determine the limiting sizes sustaining the transition. A qualitative comparison with some experimental observations is done.

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