Abstract
A microscopic theory of collective and independent·particle motion in many· fermion system is developed in the framework of the classical theory. The basic idea is an extention of the conventional time-dependent Hartree-Fock method with the use of fermion coherent state representation. Equation to determine collective path and constraints to govern the collective and the independent-particle variables are given. Hamiltonian and other physical quantities given with the original fermion variables are rewritten to the forms expressed in terms of the collective and the independent-particle variables.
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