Abstract
A phenomenological model for a strongly disordered superconductor is considered. This is a modification of the Bardeen-Cooper-Schrieffer approach for a system with random phonon-electron interaction. We show that the instability of its mean field theory cannot be fitted by a power law with a positive exponent, in contrast to a recent result based on perturbation theory.
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Communicated by T. Spencer
Supported in part by the Deutsche Forschungsgemeinschaft
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Ziegler, K. On the mean field instability of a random model for disordered superconductors. Commun.Math. Phys. 120, 177–193 (1988). https://doi.org/10.1007/BF01217961
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DOI: https://doi.org/10.1007/BF01217961