Numerical simulations of dispersion effects in chirped Gaussian and soliton pulses

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• 作者：Libor Ladányi ; Ľubomír Scholtz ; Jarmila Müllerová
• 关键词：Dispersion ; Nonlinearities ; Solitons ; Gaussian pulse ; Nonlinear Schrodinger equation ; Pulse chirp
• 刊名：Optical and Quantum Electronics
• 出版年：2017
• 出版时间：March 2017
• 年：2017
• 卷：49
• 期：3
• 全文大小：
• 刊物主题：Optics, Lasers, Photonics, Optical Devices; Electrical Engineering; Characterization and Evaluation of Materials; Computer Communication Networks;
• 出版者：Springer US
• ISSN：1572-817X
• 卷排序：49

文摘

A finite-difference method is used to solve the nonlinear Schrödinger equation. A not frequently used numerical method is developed by replacing the time end space derivate by central-difference replacements. Results from solving the nonlinear Schrödinger equation by using the numerical method called method of lines are used to simulate the propagation of Gaussian pulses in optical fibers. Gaussian input pulse was used for the analysis of dispersion effects. For the simulation was chosen the nonlinear Schrödinger equation modified for dispersion mode. Based on the changes of the chirp parameter have been achieved final shapes of transmitted Gaussian pulses. The main objective was to demonstrate the impact of the broadening factor of the pulse and also to clarify the correlation between the change in phase and frequency chirp. The main goal of this paper is to describe and simulate effects of dispersion by using short Gaussian and hyperbolic secant optical pulses. The effect of dispersion caused frequency shift which can be compensated by effect of self-phase modulation. Frequency chirp caused by the dispersion effects can be compensated by generating opposite frequency chirp with SPM effect. This compensation can lead to fundamental soliton pulse shape generation. Temporal solitons are attractive for optical communications because they are able to maintain their width even in presence of fiber dispersion. Only a fundamental soliton maintains its shape and remains chirp-free during propagation inside optical fibers.