Description of Dispersive Wave Emission and Supercontinuum Generation in Silicon Waveguides Using Split-Step Fourier and Runge-Kutta Integration Methods

<table>(a) Temporal evolution for the 1 cm long silicon waveguide without considering the effect of TPA. (b) Contrast of the input pulse and output pulse without considering the effect of TPA. The input soliton is 50 fs (FWHM), 25 W peak power hyperbolic secant soliton with order <svg height="11.375" id="M95" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 42.5625 11.375" width="42.5625" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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Advances in Mathematical Physics

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Figure 8

Figure 8: Description of Dispersive Wave Emission and Supercontinuum Generation in Silicon Waveguides Using Split-Step Fourier and Runge-Kutta Integration Methods 

Figure 8 | Description of Dispersive Wave Emission and Supercontinuum Generation in Silicon Waveguides Using Split-Step Fourier and Runge-Kutta Integration Methods 