We show that in second-order phase transformations that are induced by an i
nhomogeneous quench the density of topological defects is drastically suppr
essed as the velocity with which the quench propagates falls below a thresh
old velocity. This threshold is approximately given by the ratio of the hea
ling length to relaxation time at freeze-out, which is the instant when the
critical slowing down results in a transition from the adiabatic to the im
pulse behavior of the order parameter.