The equation of state of hot hadronic matter is obtained, by taking into
account the contribution of the massive states with the help of the resonance
spectrum τ(m)∼m3 justified by the authors in previous papers. This
equation of state is in agreement with that provided by the low-temperature
expansion for the pion intracting gas. It is shown that in this picture the
deconfinement phase transition is absent, in agreement with lattice gauge
calculations which show the only phase transition of chiral symmetry
restoration. The latter is modelled with the help of the restriction of the
number of the effective degrees of freedom in the hadron phase to that of the
microscopic degrees of freedom in the quark-gluon phase, through the
corresponding truncation of the hadronic resonance spectrum, and the decrease
of the effective hadron masses with temperature, predicted by Brown and Rho.
The results are in agreement with lattice gauge data and show a smooth
crossover in the thermodynamic variables in a temperature range ∼50 MeV.Comment: 21 pages, LaTeX, 3 postscript figure