  We consider the quantum state describing the Disoriented Chiral Condensate
(DCC) which may be produced in high energy collisions. Using the approach
suggested by Rajagopal and Wilczek to describe the amplification of the long
wavelength classical pion modes, we consider the quantum-mechanical evolution
of the initial vacuum state into the final squeezed state describing the DCC.
The obtained wave function has some interesting properties which are discussed.
