Using the effective potential approach for composite operators we have form
ulated the quantum model of the QCD vacuum. It is based on the existence an
d importance of the non-perturbative q(-4)-type dynamical, topologically no
ntrivial excitations of the gluon field configurations. The QCD vacuum is f
ound stable since the vacuum energy density has no imaginary part. We have
also proposed a method how to determine finite (but always negative) the no
n-perturbative Yang-Mills (YM) vacuum energy density, It becomes dependent
only on a scale at which non-perturbative effects become important. The qua
rk part of the vacuum energy density depends in addition on the constant of
integration of the corresponding Schwinger-Dyson equation. The value of th
e above mentioned scale is determined from the bounds for the pion decay co
nstant in the chiral limit by implementing physically well-motivated scale-
setting scheme. (C) 1999 Published by Elsevier Science B.V. All rights rese
rved.