  We discuss an extension of the dyon-anti-dyon liquid model that includes
light quarks in the dense center symmetric Coulomb phase. In this work, like in
our previous one, we use the simplest color SU(2) group. We start with a single
fermion flavor $N_f=1$ and explicitly map the theory onto a 3-dimensional
quantum effective theory with a fermion that is only U$_V(1)$ symmetric. We use
it to show that the dense center symmetric plasma develops, in the mean field
approximation, a nonzero chiral condensate, although the ensuing Goldstone mode
is massive due to the U$_A(1)$ axial-anomaly. We estimate the chiral condensate
and $\sigma,\eta$ meson masses for $N_f=1$. We then extend our analysis to
several flavors $N_f>1$ and colors $N_c>2$ and show that center symmetry and
spontaneous chiral symmetry breaking disappear simultaneously when
$x=N_f/N_c\geq 2$ in the dense plasma phase. A reorganization of the dense
plasma phase into a gas of dyon-antidyon molecules restores chiral symmetry,
but may preserve center symmetry in the linearized approximation. We estimate
the corresponding critical temperature.
