We investigate ''nonlocal'' schemes for baryogenesis at a first-order
electroweak phase transition, in which the effects of a CP-violating c
ondensate on the bubble wall propagate into the unbroken phase where t
he sphaleron rate is unsuppressed. Such a condensate exists in multi-H
iggs-boson extensions of the standard model, and may exist due to an i
nstability in the minimal standard model. In this paper we first discu
ss the general problem of determining the perturbations induced by a C
P-violating condensate, distinguishing two regimes (quantum and classi
cal). We then give an analytic treatment of quantum-mechanical reflect
ion in the thin wall regime, in which interactions with the plasma can
be neglected as a particle propagates across the wall. We focus on le
ptons because of their much weaker coupling to the plasma. We argue th
at they are likely to be accurately described by this calculation, but
quarks are not. The relative magnitude of the baryon asymmetry produc
ed for different fermions depends on their relative Yukawa couplings (
not their zero temperature masses), their transport properties, and th
eir interactions. We calculate the baryon asymmetry for various parame
ter ranges and conclude that asymmetries comparable with observations
can be generated.