  The $\epsilon$-regime of dilaton chiral perturbation theory is introduced. We
compute the dilaton mass, the chiral condensate and the topological
susceptibility in the $\epsilon$-regime, as a function of the fermion mass. The
microscopic spectral density of the Dirac operator is obtained from dilaton
chiral perturbation theory. Our main result is that the chiral condensate and
the spectral density are related to their counterparts from ordinary chiral
perturbation theory via a simple scaling relation. This relation originates
from the mass dependence of the dilaton potential, and is valid in both the
$\epsilon$-regime and the $p$-regime. In the $\epsilon$-regime, moreover, all
results agree with the universal predictions to leading order in $\epsilon$.
