  Boost-invariant (1+1) dimensional solutions for the Disoriented Chiral
Condensate (DCC) are obtained numerically, in the context of the $SU(2)_L
\otimes SU(2)_R$ non-linear sigma model at O(p^4) in the momentum expansion. We
ignore the mass terms in the Lagrangian, as we are mainly interested in the
behavior of the solutions for small values of proper time $\tau$. The solutions
obtained at O(p^4) are matched to those of O(p^2) at a late proper time $\tau
\gg 1/m_\pi$, where $m_\pi = 140$ MeV is the mass of the pion. We find that at
O(p^4) the solutions for the DCC do not have singular behavior at early proper
times $\tau \ll 1/m_\pi$. The solutions indicate that for $\tau \lsim
(0.5-0.8)$ fm the O(p^4) corrections become important. We take the sizes of the
field derivatives to be indicators of the validity of the momentum expansion.
Thus, we deduce that the O(p^4) solutions can be used to represent the
qualitative behavior of the DCC down to proper times of about 0.2 fm. Since
below $\sim 0.2$ fm the formalism is not reliable, we conclude that the
inclusion of higher order terms beyond O(p^4) is not needed to extend the
validity of the solutions to earlier proper times.
