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Beam Propagation Method Devang Parekh 3/2/04 EE290F
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Outline What is it? FFT FDM Conclusion
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Beam Propagation Method Used to investigate linear and nonlinear phenomena in lightwave propagation Helmholtz’s Equation
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BPM (cont.) Separating variables Substituting back in
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BPM (cont.) Nonlinear Schrödinger Equation Optical pulse envelope Switch to moving reference frame
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BPM (cont.) Substituting again First two-linear; last-nonlinear
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Fast Fourier Transform (FFTBPM) Use operators to simplify Solution
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Fast Fourier Transform (FFTBPM) A represents linear propagation Switch to frequency domain
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Fast Fourier Transform (FFTBPM) Solving back for the time domain Plug in at h/2
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Fast Fourier Transform (FFTBPM) Similarly for B(nonlinear) Using this we can find the envelope at z+h
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Fast Fourier Transform (FFTBPM) Three step process 1. Linear propagation through h/2 2. Nonlinear over h 3. Linear propagation through h/2
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Fast Fourier Transform (FFTBPM) Numerically solving Discrete Fourier Transform Fast Fourier Transform Divide and conquer method
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Fast Fourier Transform (FFTBPM) Cool Pictures
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Fast Fourier Transform (FFTBPM)
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Finite Difference Method (FDMBPM) Represent as differential equation Apply Finite Difference Method
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Finite Difference Method (FDMBPM)
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Cool Pictures
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Finite Difference Method (FDMBPM)
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Conclusion Can be used for linear and nonlinear propagation Either method depending on computational complexity can be used Generates nice graphs of light propagation
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Reference Okamoto K. 2000 Fundamentals of Optical Waveguides (San Diego, CA: Academic)
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