  A full implementation of the Boltzmann-Langevin equation for fermionic
systems is introduced in a transport model for dissipative collisions among
heavy nuclei. Fluctuations are injected in phase space and not, like in more
conventional approaches, as a projection on suitable subspaces. The advantage
of this model is to be specifically adapted to describe processes characterised
by instabilities, like the formation of fragments from a hot nuclear system,
and by dissipation, like the transparency in nucleus-nucleus collisions.

Nuclear Theory