Abstract

Semiclassical kinetic equations, like for example the Boltzmann-Nordheim-Vlasov (BNV) [1,2] and classical hydrodynamics [3], are used extensively to describe heavy ions collisions at intermediate and high energy [1,4]. The processes as the deep-inelastic or collective excitations are tentatively described in the Vlasov approximation [5,8] that represent the lowest order term in ħ-series expansion of the time dependent Hartree Fock equation (TDHF) [9,10]. This approximation, suitable in order to study average quantum observables or system at high entropy, washes out shell effects and neglects other typical quantum effects as tunneling and coherence.

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