The ratio of the sigma mass to the pion mass at finite temperatures and den
sities provides for a quantitative signal of chiral symmetry breaking. We c
alculate this ratio by using an extension to finite chemical potential of t
he field theoretic composite operator formalism as applied to QCD. The calc
ulation is limited to regions of the phase diagram where only quark-antiqua
rk condensates dominate (no quark-quark condensates) and it confirms the ex
pected behaviors. In particular the sigma becomes an essentially stable par
ticle in a narrow region bordering the transition line from broken to resto
red chirality. This pattern is qualitatively the same both for the region w
here the transition is of second order as for the region where it is of fir
st order (apart from the discontinuities expected in the latter case).