Abstract
A convolution form of the free energy density of the thermodynamic system of hadrons is given on the basis of the convolution formula which yields a general form of the statistical bootstrap equation. It is shown that in the thermodynamic limit this free energy density has a typical singular form, which presents a phase transition between hadronic and quark matter, in the same way as magnetic transitions and classical liquid-gas transitions. The characteristic multiplicity distribution is predicted as a signal of the disordered state.
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