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

Demonstration Of Optical Bistability By Resonant Excitation Of Nonlinear Guided Waves

Guy Vitrant, P. Arlot, R. Reinisch

Published Sep 22, 1987• 2 citations
Publisher

Abstract

A guided wave is launched through a nonlinear prism coupler whose prism-waveguide gap is filled with a liquid crystal. We observe that the intensity of the guided wave may exhibit optical bistability. Tests are realized which proove that the loops are true bistable cycles and not only hysteresis. The experimental results are in good agreement with plane-wave calculations. The disagreement with finite-width incident beam calculations is explained by a thermal averaging process within the liquid crystal.

DOI
10.1117/12.941203

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A guided wave is launched through a nonlinear prism coupler whose prism-waveguide gap is filled with a liquid crystal. We observe that the intensity of the guided wave may exhibit optical bistability. Tests are realized which proove that the loops are true bistable cycles and not only hysteresis. The experimental results are in good agreement with plane-wave calculations. The disagreement with finite-width incident beam calculations is explained by a thermal averaging process within the liquid crystal.
Utilizing prism coupling of an argon laser beam into a nonlinear ZnS waveguide we have observed power-dependent optical bistability. We detuned the incidence angle by several linewidths from the optimal low power efficiency case. At this position we observed switching and hysteresis and verified the hysteresis loop to be bistable. The origin of the bistability we tentatively identified as a combination of intensity-dependent absorption and dispersion. Our conditions for bistability were different from those of W. Lukosz et al. in OPTICAL BISTABILITY III (Springer-Verlag, New York, 1986), p. 109.
The salient question which arises when light is coupled via a grating or a prism into a waveguide exhibiting an intensity-dependent refractive index is whether switching occurs with or without bistability under appropriate detuning conditions. There are two prevailing theories. In the first1, a plane wave input is assumed leading to a uniform optically induced index change in the coupling region. In the second2, a finite width incident beam is assumed and the growth of the guided field under the coupler leads to an index change proportional to the local guided wave intensity. The first approach leads to optical bistability under certain detuning conditions, whereas the second results in switching only. Although it is known that plane wave analyses are inadequate when dealing with linear-nonlinear interfaces, bistability has been observed experimentally with nonlinear prism couplers3. Fundamentally the finite beam theoretical approaches are unable to predict bistability because no longitudinal feedback is included. Recently we showed that when non-locality is introduced into the optically induced refractive index change, longitudinal feedback occurs and bistability is predicted for the growing mode case4. However, the model used for the non-locality was artificial and resulted only in qualitative predictions. In this paper the nonlocality is modelled by the same equation used to describe heat transfer and carrier diffusion, leading to a quantitative estimate of the minimum diffusion length required for bistability.