In an oscillatory field

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

the coefficient aa multiplying the is the amplitude. It may be a complex scalar or vector. For real-valued fields one often takes Re(aeiκΦ)\operatorname{Re}(ae^{i\kappa\Phi}) or the conjugate pair aeiκΦ+aˉeiκΦae^{i\kappa\Phi}+\bar a e^{-i\kappa\Phi}; these conventions differ by a factor of two.

Separation assumptions

Calling aa an amplitude does not imply it varies slowly. Relative derivative bounds must be supplied. The decomposition also depends on convention: a phase factor can be moved between aa and the unless a choice has been fixed. An envelope is a bound on an amplitude, not necessarily the amplitude itself.