We consider extreme type-II superconductors modeled by the Ginzburg–Landau energy with a pinning term , which we assume to be a bounded measurable function such that for some constant . A crucial feature of this type of superconductors is the occurrence of vortices, which appear above the so-called first critical field . In this paper we estimate this value and characterize the behavior of the Meissner solution, the unique vortexless configuration that globally minimizes the energy below . In addition, we show that beyond this value, for applied fields whose strength is slightly below the so-called superheating field , there exists a unique Meissner-type solution that locally minimizes the energy.

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