Abstract
An a priori quantized time-dependent Hartree-Bogoliubov theory is proposed for the purpose of approaching the description of nuclear collective motion with large amplitudes. The basic idea lies in the generalization of the Schwinger representation of quasi-spin to the fermion-pair algebra, Under the c-number replacement of bosons, equations obtained in the theory are reduced to those of the time-dependent Hartree-Bogoliubov theory.

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