The multiple-scale expansion of a quasi monochromatic wave solution of
strongly dispersive and weakly nonlinear wave equations leads, in mos
t cases, to the well-known slow amplitude modulation which satisfies t
he Nonlinear Schrodinger equation. Here we consider the full expansion
, and provide a method of computing higher order effects with the cond
ition that the higher coefficients be bounded functions (no secular gr
owing in time). The integrability of the NLS equation, and the asympto
tic behaviour of its solutions, are the basic ingredients of our const
ruction. The present investigation is confined to the continuum spectr
um.