An oscillatory pulse is a field of the form

w(v,x)=χ(v)a(v,x)eiκΦ(v,x),w(v,x)=\chi(v)a(v,x)e^{i\kappa\Phi(v,x)},

where a or decay of the amplitude localizes it in the pulse coordinate vv. The phase produces rapid oscillations; a describes the amplitude's growth and decay. Additional spatial cutoffs can localize the pulse in space.

Effect of localization

Multiplying a solution amplitude by χ\chi creates a term χa\chi'a in a first-order evolution equation. It is small only if one has bounds for the amplitude where χ0\chi'\ne0. Exponential smallness near pulse endpoints can control this error; localization alone does not preserve an exact equation.