The average power spectrum of a pulse reflected by a disordered medium embe
dded in an N-mode waveguide decays in time with a power law t(-p) We show t
hat the exponent p increases from 3/2 to 2 after N-2 scattering times, due
to the onset of localization. We compare two methods to arrive at this resu
lt. The first method involves the analytic continuation to an imaginary abs
orption rate of a static scattering problem. The second method involves the
solution of a Fokker-Planck equation for the frequency dependent reflectio
n matrix, by means of a mapping onto a problem in non-Hermitian quantum mec
hanics.