  We have studied possible formation of $\Theta$ vacua states in heavy ion
collisions. Random phases of the chiral fields were evolved in a finite
temperature potential, incorporating the breaking of $U_A(1)$ symmetry. Initial
random phases very quickly settle into oscillation around the values dictated
by the potential. The simulation study indicate that an initial $\Theta$=0
state do not evolve into a $\Theta$ $\neq$ 0 state. However, an initial
$\Theta$ $\neq$ 0 state, if formed in heavy ion collision, can survive, as a
coherent superposition of a number of modes.
