We explore the effects of the proximity to a superconductor on the lev
el density of a billiard for the two extreme cases that the classical
motion in the billiard is chaotic or integrable. In zero magnetic fiel
d and for a uniform phase in the superconductor, a chaotic billiard ha
s an excitation gap equal to the Thouless energy. In contrast, an inte
grable (rectangular or circular) billiard has a reduced density of sta
tes near the Fermi level, but no gap. We present numerical calculation
s for both cases in support of our analytical results. For the chaotic
case, we calculate how the gap closes as a function of magnetic field
or phase difference.