We study the density of quasiparticle states of dirty d-wave superconductor
s, We show the existence of singular corrections to the density of states d
ue to quantum interference effects. We then argue that the density of state
s actually vanishes in the localized phase as \E\ or E-2 depending on wheth
er time-reversal is a good symmetry or not. We verify this result for syste
ms without time-reversal symmetry in one dimension using supersymmetry tech
niques. This simple, instructive calculation also provides the exact univer
sal scaling function for the density of states for the crossover from balli
stic to localized behavior in one dimension. Above two dimensions, we argue
that in contrast to the conventional Anderson localization transition, the
density of states has critical singularities which we calculate in a 2 + e
psilon expansion. We discuss consequences of our results for various experi
ments on dirty high-T-c materials. [S0163-1829(99)00833-4].