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 fro...
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Main Authors | , , |
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Format | Journal Article |
Language | English |
Published |
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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DOI: | 10.48550/arxiv.cond-mat/0508049 |