We investigate one aspect of the proximity effect, viz., the local density
of states of a superconductor-normal metal sandwich. In contrast to earlier
work, we allow for the presence of an arbitrary elastic mean free path in
the structure. The superconductor induces a gap in the normal-metal spectru
m that is proportional to the inverse of the elastic mean free path l(N) fo
r rather clean systems. For a mean free path much shorter than the thicknes
s of the normal metal we find a gap size proportional to l(N) that approach
es the behavior predicted by the Usadel equation (diffusive limit). We also
discuss the influence of interface and surface roughness, the consequences
of a nonideal transmittivity of the interface, and the dependence of our r
esults on the choice of the model of impurity scattering.