  We discuss the global symmetries of the high temperature phase of QCD with
$N_f$ massless quarks. We show that the $U(N_f) \times U(N_f)$ symmetries are
only violated by operators of dimension $\geq 3 N_f$. For $N_f > 2$ this
implies that the thermal two-point correlation functions of the $\eta'$ and
$\pi^a$'s are identical. We discuss the implications of this for the chiral
phase transition at finite temperature.
