The average phase-space density described by the Boltzmann-Langevin mo
del can largely deviate from the one provided by the Boltzmann-Uhling-
Uhlenbeck model, due to the non-linear evolution of density fluctuatio
ns. This aspect is investigated for long-wavelength, small density flu
ctuations in the framework of a memory incorporated Boltzmann-Langevin
model. It is shown that the correlations associated with density fluc
tuations yield a collision term describing coupling between the collec
tive vibrations and the single-particle degrees of freedom, which may
play an important role in damping of collective motion in both the sta
ble and unstable regions.