Abstract
The density of localised states in the low-energy tail for an electron in a gaussian random potential with long-range spatial correlations is found by evaluating instanton contributions to the n to 0 replica field representation of the one-electron Green function. It is shown that the density of states in the tail crosses over from the form mod E mod d(5-d)/4 exp(-const mod E mod 2-d/2) to the form mod E mod d exp(-const mod E mod 2) when the correlation length exceeds the de Broglie wavelength.

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