Abstract

We investigate what would happen to the time dependence of a pulse reflected by a disordered single-mode waveguide if it is closed at one end, not by an ordinary mirror, but by a phase-conjugating mirror. We find that the waveguide acts like a virtual cavity with resonance frequency equal to the working frequency ${\ensuremath{\omega}}_{0}$ of the phase-conjugating mirror. The decay in time of the average power spectrum of the reflected pulse is delayed for frequencies near ${\ensuremath{\omega}}_{0}.$ In the presence of localization the resonance width is ${\ensuremath{\tau}}_{s}^{\ensuremath{-}1}\mathrm{exp}(\ensuremath{-}L/l),$ with L the length of the waveguide, l the mean free path, and ${\ensuremath{\tau}}_{s}$ the scattering time. Inside this frequency range the decay of the average power spectrum is delayed up to times $t\ensuremath{\simeq}{\ensuremath{\tau}}_{s}\mathrm{exp}(L/l).$

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