Abstract
The confinement of optical pulses in nonlinear inhomogeneous slab waveguides is theoretically derived and parametrically investigated with a set of controlling parameters consisting of optical wavelength, slab thickness, percentage of doping, ratio of slab thickness to optical wavelength, film nonlinearity, and injected power.1,2 The model consists of a thin optical dielectric film sandwiched between semi-infinite dielectrics (substrate and cover). The three layers possess a Kerr-like nonlinearity. The electric fields, and consequently the powers trapped in each slab, are derived under simple, but accurate, forms. The confinement factor is as follows: C = Pf/(Pf + Pc + Ps), where Pf, Pc, and Ps are, respectively, the trapped power through the film, the cover, and the substrate. The correlation of C and the ratio d/λ (2d is the slab thickness and λ is the optical wavelength) is obtained under a simple series form with coefficients that depend on the set of controlling parameters. Two different slabs (AlGaAs and SiO2–GeO2) are tested and compared. Under any common set of controlling parameters, the AlGaAs waveguide possesses a high confinement coefficient compared to the GeO2–SiO2 waveguide. The ultimate confinement is obtained if the product of film refractive index and its nonlinear coefficient equals the product of the substrate.
© 1990 Optical Society of America
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