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It is shown that the effects of the charging energy on the mean-field transition temperature of a granular superconductor depend in a profound manner on the choice of the interval for the phase φ of the order parameter. For -∞<φ<∞ a well pronounced reentrant behavior is obtained for the diagonal model, in which the Coulomb interaction is neglected. The reentrance disappears in this model when the interval is taken to be -π<φ<π. Dipolar excitations of the nondiagonal model, considered recently by Efetof are shown to diminish the extent of reentrance for the -∞<φ<∞ model and to produce a weak reentrance in the -π<φ<π case. The reentrant behavior is shown to be due to the thermally induced phase coherence via the low-lying excited states characterized by the vanishing of the frequency of the phase rotation.
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E. Šimánek (1981) studied this question.
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