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AIP conference proceedings

Quantum initiation effects on the asymptotic coherent on-resonance propagation of two different-wavelength probe and pump beams in a three-level system

Farrès P. Mattar, Yves Claude, M. Burgess

Published Jan 1, 1989• 0 citations
Publisher

Abstract

The coherent energy transfer from a strong pump beam at a given frequency to a weak probe beam initiated by quantum noise at another frequency is reported. Effects of self‐ and cross‐phase modulation were also examined. An optimal energy exchange is maintained in the presence of fluctuations by matching the oscillators strengths to insure maximum pulse overlap throughout the motion. The central role of pump depletion, transverse effects, quantum initiation and time‐ and radial‐dependent phase variations in an asymptotic co‐propagation in a three‐level medium is revealed. An ensemble of statistical calculations is carried out. For most trajectories a stabilization of the pulse area is inhibited. Probe pulse sharpening and pump laser pulse peak retardation along with amplitude dimension, have been observed.

DOI
10.1063/1.38550

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AIP conference proceedings•Jan 1, 1989•0 citations
The coherent energy transfer from a strong pump beam at a given frequency to a weak probe beam initiated by quantum noise at another frequency is reported. Effects of self‐ and cross‐phase modulation were also examined. An optimal energy exchange is maintained in the presence of fluctuations by matching the oscillators strengths to insure maximum pulse overlap throughout the motion. The central role of pump depletion, transverse effects, quantum initiation and time‐ and radial‐dependent phase variations in an asymptotic co‐propagation in a three‐level medium is revealed. An ensemble of statistical calculations is carried out. For most trajectories a stabilization of the pulse area is inhibited. Probe pulse sharpening and pump laser pulse peak retardation along with amplitude dimension, have been observed.
The coherent frequency conversion between on‐resonance pump and probe beams is examined in the physical situation where the nonlinear gain balances the diffraction for the probe transition. The semiclassical paraxial‐Maxwell‐Bloch formalism is adopted as introduced in propagational studies in two‐level Self‐Induced‐Transparency (SIT)[1]. The probe builds up from an input deterministic seed. The asymptotic stabilization of the probe area is reported in conjunction with pump depletion and diffraction rigorously accounted for. Without diffraction the soliton does not appear. The Laplacian term (which describes transverse coupling) is included.
The coherent frequency conversion between on-resonance pump and probe beams is examined in the physical situation where the medium nonlinearity balances the linear diffraction for each transition. Without diffraction neither soliton can occur. The paraxial-Maxwell Bloch formalism is adopted. To achieve optimally the energy transfer the pulse velocities must be equal to maintain maximum overlap throughout the propagation. The sequential evolution of probe soliton then pump soliton is reported in conjunction with pump depletion diffraction rigorously accounted for. Phase diagram of the pump and probe areas exhibit multi-value features.
Analytic and numerical calculations for the propagational dependence of Rabi-Split resulting from a strong resonant pump and a coupled weak off-resonance probe are presented for a Lambda three-level atomic configuration. A semi-classical Maxwell-Bloch formulism was adopted for both the perturbational (using stationary phase and steepest descent asymptotic techniques) and the rigorous computational treatments. This calculation can be considered as a Double Self-Induced Transparency SIT' where the strong pump (multiple of 2n on-axis area) experiences coherent pulse break up, coherent self-focusing 2-4 and depletion as the weak probe (multiple of 0.02n area) cooperatively builds up. Different transition gain ratios (i.e., oscillator strength: p2w) are considered to insure that the weak probe does not get (a) delayed with respect to the pump or (b) get out of synchronization, and cease to overlap. The probe detuning can be as large as the input on-axis pump Rabi frequency. The interplay of nonlinear Raman gain action, dispersion and diffraction give rise concommitantly to a number of effects previously studied independently such as self-phase modulation, wave front encoding, transverse ring formation, self-focusing, quasi-trapping (when pump detuning is also allowed), and asymptotic three-level solitary waves.