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AIP conference proceedings

Transverse on-resonance asymptotic reshaping in coherent probe soliton formation in a three-level system

Farrès P. Mattar

Published Jan 1, 1988• 0 citations
Publisher

Abstract

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.

DOI
10.1063/1.37408

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The goal of this communication is to show that different transmission characteristics are obtained for each pulse shape when diffraction is accounted for even if the time‐integrated areas are equal. For weakly overlapped two‐field propagation it was argued that each pulse evolution obeys its own area theorem. In our case the pulses are strongly overlapped and they mutually influence each other. We have worked out the transverse variation beyond the physical situation where a specific self‐similar Gaussian mode can be assumed. Detailed temporal and frequency reshaping of coherent pulses with finite beam extent in a three‐level absorber is reported.

AIP conference proceedings•Jan 1, 1988•0 citations
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.
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.
A computer movie illustrating a rigorous multimode calculation of SF, St, Prb buildup in Raman studies is presented. This coherent copropagational study based on Maxwell-Bloch formalism1 includes phase and transverse variations, nonlinear asymmetric dispersion, pump spatial depletion, and time-dependent variations in population inversion density. Theλ scheme is selected so that the active transitions are optically thick for both the pump (α p l > 5) and the SF (α sf l > 35) pulses. This choice of Beer lengths, i.e., of oscillator strengths, insures that the two pulses never cease to overlap and optimizes the SF initially small signal growth. The pump interacts like a self-induced transparency while the SF, St, Prb evolves as a small-area in a two-level emitter which can be described as a nonlinear pendulum in the pane wave. For a given ratio of Beer lengths, distinct Fresnel numbers, atomic density numbers, small signal SF, St, Prb time-integrated energy stabilization or self-focusing may arise, as observed experimentally. For a sufficiently larger propagation distance, an asymptotic evolution of a quasisolitary nonhyperbolic-secant pulse of constant area is reported.
The goal of this communication is to show that different transmission characteristics are obtained for each pulse shape when diffraction is accounted for even if the time‐integrated areas are equal. For weakly overlapped two‐field propagation it was argued that each pulse evolution obeys its own area theorem. In our case the pulses are strongly overlapped and they mutually influence each other. We have worked out the transverse variation beyond the physical situation where a specific self‐similar Gaussian mode can be assumed. Detailed temporal and frequency reshaping of coherent pulses with finite beam extent in a three‐level absorber is reported.