Abstract
We have calculated the density of states of superconducting spheres much smaller in size than the coherence length ξ0 and the penetration depth λ for arbitrary mean free path l and arbitrary fields at zero temperature. In agreement with experimental results, the theory predicts an appreciable deviation from results obtained in the limit l0 even if the ratio lξ0 is small, like lξ00.1. We also discuss the dependence of the critical field on the mean free path and the boundary condition for arbitrary temperatures.