  We investigate the possibility of parity being spontaneously violated in QCD
at finite baryon density and temperature. The analysis is done for an idealized
homogeneous and infinite nuclear matter where the influence of density can be
examined with the help of constant chemical potential. QCD is approximated by a
generalized sigma-model with two isomultiplets of scalars and pseudoscalars.
The interaction with the chemical potential is introduced via the coupling to
constituent quark fields as nucleons are not considered as point-like degrees
of freedom in our approach. This mechanism of parity violation is based on
interplay between lightest and heavier degrees of freedom and it cannot be
understood in simple models retaining the pion and nucleon sectors solely. We
argue that, in the appropriate environment (dense and hot nuclear matter of a
few normal densities and moderate temperatures), parity violation may be the
rule rather than the exception and its occurrence is well compatible with the
existence of stable bound state of normal nuclear matter. We prove that the so
called 'chiral collapse' never takes place for the parameter region supporting
spontaneous parity violation.
