Abstract
Fluctuation-induced diamagnetism (FID) above the critical temperature is considered via the superconductive glass (SG) model. The model predicts a crossover between two-and three-dimensional behaviours of FID. It is shown that for temperatures well above T c a two-dimensional analog of the Aslamazov-Larkin law is realized, while in the region near T c FID reduces to a three-dimensional form of the XY-like model of a granular superconductor.
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