The microscopic dynamics of a quantum many-body system is analyzed und
er the assumption that numerous complicated intermediate states in exa
ct operator equations of motion are of chaotic nature and can be avera
ged out. The averaging procedure, preserving all kinematical constrain
ts, is defined by the invariance with respect to phase transformations
. The situation with no significant collective correlations is conside
red in detail. As a result, the mean-field theory (MFT) emerges accumu
lating the smooth component of the total random dynamics. The obtained
version of the MFT differs from the Hartree-Fock approximation in tak
ing into account the average effect of fluctuations. The mean-field re
presentation is suggested to be a natural basis for estimating the deg
ree of complexity of generic complicated wave functions.