Migdal's theory of finite Fermi systems is applied for the description
of nucleus-nucleus collisions at laboratory energies less than a few
GeV/A. It is taken into account that the pionic degree of freedom soft
ens in nuclear matter. Free paths of nucleon and pion quasiparticles a
re calculated. Compact formulas are written for pion, nucleon- and pho
ton-production cross sections. In addenda, the main formulas are prese
nted for the NN-interaction amplitude and pion polarization operator i
n non-equilibrium and heated equilibrium nuclear matter.