The possibility of producing quark-gluon plasma in
relativistic heavy ion collisions is an exciting
one, especially from the point of view of
observing the chiral phase transition as the
hot plasma expands and cools.
As the system returns to normal phase
it is possible for regions of misaligned vacuum
to be produced. These domains which are analogous
to misaligned domains of a ferromagnet have
been named Disoriented Chiral Condensates (DCCs). If
we parametrize the condensate using the
chiral field
which in the ground state
takes the value (v,0), the DCC's are regions
where the chiral field is partially aligned
in the pion directions. These domains could
behave as ``pion lasers'' and emit pions and therefore
we will probably be able to detect them. A great
amount of recent work is devoted to the study
of DCC's, since a better understanding of the relevant
physics could shed some light on the most general
problem of the QCD phase transition.