On the basis of a canonical formulation of full time-dependent Hartree-Fock method, we develop a formulation of time-dependent Hartree-Fock method for the description of collective motion in a completely canonical form.In the derivation of basic equations, the general form of canonicity condition plays an important role.
A microscopic theory of collective and independent-particle motions in many-fermion system is developed in the framework of Dirac's canonical theory with constraints.The basic idea is an extension of the conventional time-dependent Hartree-Fock theory based on the use of the Grassmann variables and, in certain sense, it supplements incomplete parts of the paper presented by the present authors.Canonicity condition to certify the canonical property of the variables, equation to determine collective submanifold and constraints to govern the collective and the Grassmann variables are given.
From the viewpoint defferent from that of Part I, the time-dependent Harteree-Fock theory is formulated for describing large amplitude collective motion and its coupling with intrinsic degrees of freedom. The basic idea consists of the introduction of an additional degree of freedom for the collective motion and the use of Dirac’s canonical theory with constraints. The formalism is essentially equivalent to the ordinary time-dependent Hartree-Fock theory presented in Part I. The result given in Part I is completely reproduced.
It is shown that the ordinary framework of (adiabatic) time-dependent Hartree-Fock method can uniquely specify the collective submanifold and its canonical coordinate system, with the aid of the RPA and the canonicity condition. Some criticism is given to the pesimistic viewpoint concerning the unique specification of collective submanifold within the adiabatic time-dependent Hartree-Fock method. A decisive foundation of the approach developed by Marumori, Maskawa, Sakata and one of the present author (A. K.) is given.