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time-dependent Hartree-Fock equation; nuclear matter
We consider an effective model of nuclear matter including spin and isospin degrees of freedom, described by an $N$-body Hamiltonian with suitably renormalized two-body and three-body interaction potentials. We show that the corresponding mean-field theory (the time-dependent Hartree-Fock approximation) is ``exact'' as $N$ tends to infinity.
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