Abstract
According to the pioneering model proposed by Nambu and Jona-Lasinio (NJL) \cite{2,3}, a massless fermion acquires its mass via a vacuum phase transition (VPT) process. Our discussion is considerably simplified because an effective Hamiltonian for VPT is proposed and a simple regularization-renormalization method (RRM) is adopted. An unambiguous constraint is found as , where is the coupling constant first introduced in the NJL model while the mass of fermion () created after the VPT. The masses of bosons with spin-parity and as collective modes composed of fermion-antifermion pairs (s) are also calculated by the method of random phase approximation (RPA).
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