The composite operator formalism is applied to QCD at finite temperature to
calculate the masses of scalar and pseudoscalar mesons. In particular the
ratio of the sigma mass to the pion mass is an interesting measure of the d
egree of chiral symmetry breaking;It different temperatures. We calculate t
he temperature T* at which M-sigma(T)less than or equal to 2M(pi)(T), above
which the sigma partial width into two pions vanishes. We find T* = 0.95T(
c). (where T-c is the critical temperature for the chiral phase transition)
, within the full effective potential given by the formalism. We find that
an expansion a la Landau of the effective potential around the critical poi
nt in the limit of small quark mass provides for a very good determination
of T*. [S0556-2821(99)05411-9].