For the factor eiΨ(t,x)e^{i\Psi(t,x)}, the local wavevector is

k(t,x)=xΨ(t,x).k(t,x)=\nabla_x\Psi(t,x).

If Ψ=κΦ\Psi=\kappa\Phi with constant κ\kappa, then k=κΦk=\kappa\nabla\Phi. The points normally to the local constant-phase surfaces where it is nonzero.

Plane waves and conventions

For ei(k0xωt)e^{i(k_0\cdot x-\omega t)}, the wavevector is the constant k0k_0. In the convention e2πiξxe^{2\pi i\xi\cdot x}, it is 2πξ2\pi\xi. Thus a Fourier frequency measured in cycles per unit length and an angular wavevector differ by 2π2\pi.