Hadronization in SU(N) Gauge Field Theory

Abstract

The bosonization of the strong interacting matter as a process of arising observable hadrons is studied in terms of the phase transition of the second kind. The spectrum of bosons which is free from the zero point energy is derived . The calculated boson mass is found to depend selfconsistently on both the amplitude of a gauge field and quark mass. In the framework of the quasi-classical model[10, 11] a hadron mass is calculated in the case of bosonization into pions.