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Bosonization of the strong interacting matter as a process of arisingobservable hadrons is studied in terms of the phase transition of the secondkind. The spectrum of bosons which is free from the zero point energy isderived . The calculated boson mass is found to depend self-consistently onboth the amplitude of a gauge field and quark mass. In the framework of thequasi-classical model a hadron mass is calculated in the case of bosonizationinto pions.

Bosonization in SU(N) Gauge Field Theory in Terms of Phase Transition of Second Kind