  We argue that disoriented chiral condensate (DCC) domains are not well
defined for temperatures above the Ginzburg temperature $T_G$ ($\simeq 0.7
T_c$). Above $T_G$, the dynamics of DCC domains is dominated by thermal
fluctuations leading to fluctuating orientation of the chiral field in a given
domain. It implies that DCC domains may form even in relatively lower energy
collisions where the temperature only reaches $T_G$, and never rises to $T_c$.
It also means that detection of DCC can not be taken as a signal for an
intermediate chirally symmetric phase of matter. Using these considerations, we
estimate the probability distribution for DCC domains as a function of the
chiral angle.
