We study the detailed out-of-equilibrium time evolution of a homogeneous Bo
se-Einstein condensate (BEC). We consider a nonrelativistic quantum theory
for a self-interacting complex scalar field, immersed in a thermal bath, as
an effective microscopic model for the description of the BEG. The interac
tion between fluctuations proves to be crucial in the mechanism of instabil
ity generation. We show the existence of two regimes in k space, with a cro
ssover for k(2)/2m similar to 2 lambda\phi(0)\(2), where lambda is the coup
ling constant and \phi(0)\(2) is the condensate density. We deduce and solv
e a set of coupled equations that completely determines the nonequilibrium
dynamics of the condensate density.