Abstract
The Beam Propagation Method (BPM) has been used extensively to model propagation in optical fibers [1,2]. In this paper we extend this technique to model propagation in the presence of a second and third order nonlinear susceptibility in the glass. Using this technique, nonlinear effects such as second harmonic generation (SHG), self phase modulation (SPM) and cross phase modulation (XPM) can be modeled.
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