Abstract

We present here some fundamental but yet underlooked features of the propagation of weak ultrashort pulses (with Δ d τ << 1, where Δ d is the Doppler width and τ is the pulse duration) in resonant atomic media. We show that the pulse area behaviour and the pulse spectrum at resonance are governed by the usual optical depth ( α 0 L, where α 0 is the absorption coefficient at resonance and L the length of the medium), whereas the pertinent parameter that governs the severity of the dispersion effects and the distortion of the pulse is the dispersion parameter e disp = ( α 0 L) Δ d τ that we introduce. Paradoxical effect such as distortionless propagation (e.g. e disp << 1) with vanishing pulse area (when α 0 L >> 1) can then explained within this formalism.

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