We have a wave ψ(x,z,t). At t = 0 we can assume the wave to have the solution (and shape)
ψ = Q*exp[-i(kx)]
where k = wavenumber, i = complex number
The property for a Fourier transform of a time shift (t-τ) is
FT[f(t-τ)] = f(ω)*exp[-i(ωτ)]
Now, assume ψ(x,z,t) is shifted in time...