A Hamiltonian difference scheme associated with the integrable nonline
ar Schrodinger equation with periodic boundary values is used as a pro
totype to demonstrate that perturbations due to truncation effects can
result in a novel type of chaotic evolution. The chaotic solution is
characterized by random bifurcations across standing wave states into
left and right going traveling waves. In this class of problems where
the solutions are not subject to even constraints, the traditional mec
hanism of crossings of the unperturbed homoclinic orbits/manifolds is
not observed.