We construct a generally applicable short-time perturbative expansion
for coherence loss. Successive terms of this expansion yield character
istic times for decorrelation processes involving successive powers of
the Hamiltonian. The second order results are sufficient to precisely
reproduce expressions for ''decoherence times'' obtained in the liter
ature by much more involved and indirect methods. Examples illustratin
g the influence of initial conditions and the need to evaluate higher
order terms are given in the context of the Jaynes-Cummings model. It
is shown that, in this case, the short-time decoherence behavior can p
robe the importance of antiresonant contributions.