1996
DOI: 10.1002/sapm1996972127
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Coherent Structures in Weakly Birefringent Nonlinear Optical Fibers

Abstract: This article studies two coupled nonlinear Schrodinger equations that govern the pulse propagation in weakly birefringent nonlinear optical fibers. The coherent structures for these equations, such as vector solitons and localized oscillating solutions, are studied analytically and numerically. Three types of localized oscillating structures are identified and their functional forms determined by perturbation methods. In some of these structures, infinite oscillating tails are present. The implications of thes… Show more

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Cited by 13 publications
(4 citation statements)
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“…Tan and Liu [19] and Tan [17] have derived this system for applications in geophysical fluid dynamics. The coupled-NLS has also been extensively studied in nonlinear optics where only a partial list of references includes [12,28,20,13,21,15,11,1,10,27,23,24,25,26].…”
Section: Introductionmentioning
confidence: 99%
“…Tan and Liu [19] and Tan [17] have derived this system for applications in geophysical fluid dynamics. The coupled-NLS has also been extensively studied in nonlinear optics where only a partial list of references includes [12,28,20,13,21,15,11,1,10,27,23,24,25,26].…”
Section: Introductionmentioning
confidence: 99%
“…(32), v grows to finite amplitude and gradually changes its shape. Yang [19] has computed the first order corrections to these Legendre modes, but numerical methods are needed to accurately trace the full solution branch emerging from these "father-daughter" solutions. The u soliton is the "father"; the infinitesimal amplitude v, solving the Associated Legendre equation, is the "daughter".…”
Section: Father-daughter Approximationsmentioning
confidence: 99%
“…Stability analyses [18][19][20] suggest that the other species of solitary waves are easily disassociated. The equal-frequency solitary waves are merely one point on a branch of solutions, but it is when the solitary waves have equal width and frequency that they are likely to have the strongest and most varied interactions.…”
Section: Solution Branchesmentioning
confidence: 99%
“…When n = 1, (1) is referred to as the cubic nonlinear Schrödinger (NLS) equation. It has been used extensively to model, among many other applications, waves in deep water [1,37,54], propagation in nonlinear optics [28,34,53], Bose-Einstein condensates [2,25,26,36,43,49], and electron plasma waves [12]. The interaction matrix α = (α jk ) n j,k=1 contains information about the nature of the interactions between the different components of the wave functions.…”
Section: Introductionmentioning
confidence: 99%