1983
DOI: 10.1016/0030-4018(83)90095-0
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Soliton analysis with the propagating beam method

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Cited by 66 publications
(16 citation statements)
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“…This equation describes the combined effect of dispersion and nonlinearity on the pulse inside the fiber. It can be numerically solved using Split Step Fourier Transform (SSFT) [10], [12]. The dispersion is responsible for temporal broadening of the pulse and in particular anomalous dispersion leads to negative chirp across the input pulse.…”
Section: Non-linear Pulse Propagation In Optical Fibersmentioning
confidence: 99%
“…This equation describes the combined effect of dispersion and nonlinearity on the pulse inside the fiber. It can be numerically solved using Split Step Fourier Transform (SSFT) [10], [12]. The dispersion is responsible for temporal broadening of the pulse and in particular anomalous dispersion leads to negative chirp across the input pulse.…”
Section: Non-linear Pulse Propagation In Optical Fibersmentioning
confidence: 99%
“…In most cases, (1) and its modifications cannot be solved analytically and one has to use numerical approaches. Here we will use the most commonly applied numerical scheme for solving the NLSE, the so-called split-step Fourier transform (SSFT) method [13]. In order to characterize the fiber distances over which dispersive and nonlinear effects are important, two parameters are usually used, namely, the dispersion length L D and the nonlinear length L NL , [1] …”
Section: Theoretical Fundamentsmentioning
confidence: 99%
“…In case of BPM the pulse shape after completing A segment q( + A) is expressed as a function of the input pulse q(C) by the expression [9]: q(r, C+AC)= G. H(G . q(r, ç))G. g(v, )+o(Aç3).…”
Section: Introductionmentioning
confidence: 99%