  A thermal Finite Energy QCD Sum Rule is used to determine the temperature
behaviour of the $\omega \rho \pi$ strong coupling. This coupling decreases
with increasing $T$ and vanishes at the critical temperature, a likely signal
for quark deconfinement. This is then used in the Vector Meson Dominance (VMD)
expression for the $\pi^0 \to \gamma \gamma$ amplitude, which is also found to
vanish at the critical temperature, as expected. This result supports the
validity of VMD at $T \neq 0$. However, if VMD would not hold at finite
temperature, then there is no prediction for the $\pi^0 \to \gamma \gamma$
amplitude.
