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 Malbouisson, A. P. C, Milla, Y. W, Roditi, I
Format Journal Article
LanguageEnglish
Published 01.08.2005
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Abstract 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.
AbstractList 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.
Author Milla, Y. W
Roditi, I
Malbouisson, A. P. C
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BackLink https://doi.org/10.1016/j.physa.2005.05.082$$DView published paper (Access to full text may be restricted)
https://doi.org/10.48550/arXiv.cond-mat/0508049$$DView paper in arXiv
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Snippet 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...
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SubjectTerms Physics - Superconductivity
Title Gauge fluctuations and transition temperature for superconducting wires
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