Boltzmann-Langevin One-Body dynamics for fermionic systems

Abstract

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.

Comments: Conf. proc. 105, IWM2011 http://dx.doi.org/10.1051/epjconf/20123100027