An efficient way of third-order dispersion compensation for reshaping parabolic pulses through normal dispersion fiber amplifier

被引:2
作者
Chowdhury, Debasruti [1 ]
Ghosh, Dipankar [2 ]
Basu, Mousumi [1 ]
机构
[1] Indian Inst Engn Sci & Technol, Dept Phys, Howrah 711103, W Bengal, India
[2] MCKV Inst Engn, Dept Basic Sci, Howrah 711204, W Bengal, India
关键词
third-order dispersion; nonlinear Schrodinger equation; parabolic pulse; similariton; time-reversal system; time-flipping technique; critical length; OPTICAL-TRANSMISSION SYSTEMS; SPECTRAL PHASE-CONJUGATION; GROUP-VELOCITY DISPERSION; SELF-SIMILAR PROPAGATION; TIME LENSES; DECREASING FIBER; WAVE-BREAKING; GENERATION; SIMILARITONS; REVERSAL;
D O I
10.1088/2040-8986/aad829
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Normal dispersion decreasing fibers (NDDFs) employed for parabolic pulse (PP) generation are limited by the presence of inherent third-order dispersion (TOD), which leads to distortion in pulse shape from its parabolic nature. This necessitates a compensation method for TOD for such fibers. Dispersion-compensating fiber (DCF) amplifiers with relatively smaller values of dispersion can also be largely affected by this harmful effect of TOD when used for the same purpose. As a solution, a time-reversal system (TRS) based on a time-conjugating technique is employed with the aim of minimizing the deleterious effects of TOD. A detailed study on the estimation of the critical length where the time lens system needs to be implemented within the fiber link is crucial for reshaping the pulse into parabolic form. An NDDF is designed and optimized to possess a relatively higher value of TOD and a cascaded fiber optic system comprising the first stage of the proposed NDDF, the TRS and the second stage of the NDDF is suggested here to obtain linearly chirped PP at the output end even in the presence of a high value of TOD. The proposed scheme has also proved to be efficient for better pulse reshaping through DCFs possessing a high amount of TOD.
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页数:11
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