Coupled-mode theory of diffraction-induced transverse effects in nonlinear optical resonators

R. Reinisch, G. Vitrant, and M. Haelterman
Phys. Rev. B 44, 7870 – Published 15 October 1991
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Abstract

We develop a one-dimensional theory of diffraction-induced transverse effects in nonlinear Fabry-Pérot resonators addressed by finite-width incident beams. This is achieved in the framework of the coupled-mode analysis, which takes full advantage of the fact that nonlinear Fabry-Pérot devices are resonant. As compared with a recently published theory dealing with the same subject [M. Haelterman, Opt. Commun. 75, 165 (1990); M. Haelterman, G. Vitrant, and R. Reinisch, J. Opt. Soc. Am. B 7, 1309 (1990); and G. Vitrant, M. Haelterman, and R. Reinisch, ibid. 7, 1319 (1990)], where the nonlinearity is introduced in an approximate way, the formalism developed here takes the nonlinearity associated with the optical Kerr effect rigorously into account. This feature has an important consequence: It leads to a theory that can be generalized to the TM case and also to anisotropic nonlinear media. The theory presented here is valid for any value of the angle of incidence. Under normal (or quasinormal) incidence, two counterpropagating modes, having the same absolute value of the wave-vector component parallel to the plane of the mirrors, are resonantly (or nearly resonantly) excited, whereas under oblique incidence, only one of these modes is excited.

This allows us to point out that the feedback leading to optical bistability occurs along the direction of propagation of these resonantly excited counterpropagating modes of the nonlinear optical resonator. This explains why optical bistability disappears under oblique incidence. Although developed in the case of nonlinear Fabry-Pérot resonators, this theory applies to a wide range of nonlinear optical resonators such as nonlinear prism couplers, nonlinear grating couplers, nonlinear interference filters, etc. The theory developed here applies whenever the excited electromagnetic field can be accurately described by a single mode or two counterpropagating modes of the nonlinear device. As an example, numerical results are given in the case of a nonlinear multiple-quantum-well Fabry-Pérot-type structure of Al1xGaxAs/GaAs with Al1xGaxAs/AlAs mirrors.

  • Received 21 June 1991

DOI:https://doi.org/10.1103/PhysRevB.44.7870

©1991 American Physical Society

Authors & Affiliations

R. Reinisch and G. Vitrant

  • Laboratoire d’Electromagnétisme, Microondes et Optoélectronique, Ecole Nationale Supérieure d’Electronique et de Radioélectricité de Grenoble, Boîte Postale 257, 38016 Grenoble CEDEX, France

M. Haelterman

  • Service d’Optique Théorique et Appliquée, Université Libre de Bruxelles, 50 avenue F. D. Roosevelt, Code Postale 194/5, B-1050 Brussels, Belgium

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Vol. 44, Iss. 15 — 15 October 1991

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