We consider quantum effects in a world with two coexisting symmetry ph
ases, unbroken and spontaneously broken, as a result of a first order
phase transition. The discrete symmetries of the problem are discussed
in general. We compute the exact two-point Green function for a free
fermion, when a thin wall separates the two phases. The Dirac propagat
or displays both massive and massless poles, and new CP-even phases re
sulting from the fermion reflection on the wall. We discuss the possib
le quark-antiquark CP-asymmetries produced in the Standard Model (SM)
for the academic T = 0 case. General arguments indicate that an effect
first appears at order alpha(w) in the reflection amplitude, as the w
all acts as a source of momentum and the on-shell one-loop self-energy
cannot be renormalized away. The asymmetries stem from the interferen
ce of the SM CP-odd couplings and the CP-even phases in the propagator
. We perform a toy computation that indicates the type of GIM cancella
tions of the problem. The behaviour can be expressed in terms of two u
nitarity triangles.