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Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE

Coherent Resonant Pulse Propagation In A Nonlinear Absorber

G. E. Torres-Cisneros, Javier J. Sanchez-Mondragon

Published Jan 1, 1987• 0 citations
Publisher

Abstract

The nonresonant propagation of a laser pulse through a nonlinear dielectric is now a well studied subjet because its extensive and direct applications mainly in communications by means of optical fibers and in spectroscopy. On the other hand, the coherent resonant interaction between high intense laser pulses and atoms or molecules is an intrinsic nonlinear phenomena that have received a great deal of attention since the discovery of Self Induced Transparency (SIT). However, the simultaneous consideration of both sources of nonlinearities, that may represent more realistic and important experimental situations, have not been yet studied in a systematic way.

DOI
10.1117/12.967246

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The nonresonant propagation of a laser pulse through a nonlinear dielectric is now a well studied subjet because its extensive and direct applications mainly in communications by means of optical fibers and in spectroscopy. On the other hand, the coherent resonant interaction between high intense laser pulses and atoms or molecules is an intrinsic nonlinear phenomena that have received a great deal of attention since the discovery of Self Induced Transparency (SIT). However, the simultaneous consideration of both sources of nonlinearities, that may represent more realistic and important experimental situations, have not been yet studied in a systematic way.
Resonant absorption in a laser pulse can be reduced to zero if the trailing part induces stimulated emission and returns the absorbed energy back to the pulse. This kind of effect is called Self-Induced Transparency (SIT). Analytic descriptions of short pulse propagation in a resonant medium, based on Slowly Varying Envelope Approximation (SVEA) and in linear media, have been extended in studies of SIT along two principal directions: First, to improve the SVEA by introducing Short Pulse Approximation (SPA); and second, to consider the effect of nonlinear refractive index.
Self-induced transparency (SIT) is a kind of coherent transient phenomena in two-level atomic system. The optical pulse with an area that is an integer multiple of 2π, which causes SIT in an absorber, is stable and a kind of soliton. Thus SIT is expected to be useful in pulse compression and pulse shaping. In this paper, we discuss some problems in experiments of SIT and surveys the experimental results of SIT. It is also described the recent experimental results of coherent nonlinear pulse propagation in BiI3 crystal using tunable sub-picosecond pulses.
Our recent studies of methods for obtaining ultrashort light pulses and analysis of the impact of ultrashort optical pulses on classical and quantum micro-objects with the identification of the determining role of the degree of unipolarity of pulses (maximum for strictly unipolar pulses) in the efficiency of direct laser acceleration of charged particles and excitation of atoms and molecules have been reviewed. Special attention has been paid to the coherent mode locking regime in lasers, which is implemented when the laser pulse duration is less than the relaxation time of the working transition in media with resonance amplification and absorption (laser analog of the phenomenon of self-induced transparency). Experimental data on coherent mode locking in a titanium-sapphire laser with a cell with rubidium vapor at self-induced transparency in rubidium have been presented. The interaction of ultrashort pulses in resonant media has also been analyzed.
The recent development of the EDFA (erbium-doped fiber amplifier) offers the possibility for uses of the fibers to experiments on coherent pulse propagation such as self-induced transparency (SIT). The guiding of the radiation by the fiber structure eliminates diffraction effects and makes possible the interaction of the radiation with the fiber medium which has resonance effects over long distances. To date, however, experiments on SIT solitons have suffered from diffraction effects that were further complicated by nonlinear interactions. In the present paper, we report for the first time the observation of SIT soliton propagation in an erbium- doped resonant fiber waveguide.
A review is given of the investigations of the coherent interaction of light pulses with resonantly absorbing two-level media. An analysis is made of the self-induced transparency discovered by McCall and Hahn and of its importance in quantum electronics. Bleached states associated with the phase modulation are considered in detail. A comparison is made with the theory of nonlinear waves of different physical origin. A review is given of some possible physical applications associated with the discriminatory nature of the transmission and delay of light in the self-induced transparency effect.
This thesis presents theoretical models and results of numerical simulations describing the propagation of optical pulses through dense, thermal atomic vapours. In particular we investigate the nonlinear effects of optical solitons due to self-induced transparency (SIT) in two-level systems, optical simultons in V-type three-level systems and electromagnetically induced transparency (EIT) in Λ-type systems, including the storage and retrieval of dark-state polaritons. An investigation is made into two-photon excitation of the 5D states of rubidium in a high-intensity beam including the hyperfine structure of the relevant atomic levels. Decay from these states to the 6P manifolds is ruled out as a cause of experimentally observed fluorescence due to the amount of power broadening associated with intensities necessary to provide any significant level of population in these highly excited states. We combine the nonlinear effects of optical solitons and EIT to explain experimentally observed steepened pulses in a V-type system in a micron-length cell. We explain the behaviour as the early formation of a simulton pulse drawn from a CW probe field by a strong coupling pulse, due to coherent population trapping. We predict that in a longer cell it may be possible to facilitate propagation of matched pulses, even when the transitions in the system have different propagation coefficients, as long as decoherence from collision broadening can be controlled. The fact that weak pulses can propagate with this scheme suggests an approach to achieving transparent propagation of single or few photon pulses distinct from, but related to, both SIT and EIT.