2013
DOI: 10.1103/physreve.88.032903
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Rotation of the trajectories of bright solitons and realignment of intensity distribution in the coupled nonlinear Schrödinger equation

Abstract: We revisit the collisional dynamics of bright solitons in the coupled Nonlinear Schrödinger equation. We observe that apart from the intensity redistribution in the interaction of bright solitons, one also witnesses a rotation of the trajectories of bright solitons . The angle of rotation can be varied by suitably manipulating the Self-Phase Modulation (SPM) or Cross Phase Modulation (XPM) parameters.The rotation of the trajectories of the bright solitons arises due to the excess energy that is injected into t… Show more

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Cited by 15 publications
(9 citation statements)
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References 26 publications
(23 reference statements)
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“…is the transformed field and σ = Φ 0 Λ Φ −1 0 and Φ 0 is a known solution of the linear system (5), we apply the DT on the linear system given by Eqs. (4), and the stipulation that the transformed linear system be covariant with the original one requires…”
Section: Darboux Transformation With Zero Seed: Single Soliton Solutionmentioning
confidence: 99%
See 2 more Smart Citations
“…is the transformed field and σ = Φ 0 Λ Φ −1 0 and Φ 0 is a known solution of the linear system (5), we apply the DT on the linear system given by Eqs. (4), and the stipulation that the transformed linear system be covariant with the original one requires…”
Section: Darboux Transformation With Zero Seed: Single Soliton Solutionmentioning
confidence: 99%
“…UAK and PSV acknowledge the support of UAE University through the grant UAEU-UPAR (7) and UAEU-UPAR (4). RR wishes to acknowledge the financial assistance received from Department of Atomic Energy-National…”
Section: Acknowledgementsmentioning
confidence: 99%
See 1 more Smart Citation
“…For condensates in a time independent harmonic trap, λ(t) = λ 0 (a constant), Equation (11) yields γ(t) = γ 0 exp (λ 0 t), where γ 0 is an arbitrary constant. Considering a vacuum seed solution, i.e., q 1 (x, t) = q 2 (x, t) = 0, and employing gauge transformation approach [39][40][41][42], we obtain…”
Section: The Model and Lax Pairmentioning
confidence: 99%
“…where q i (x, t)(i=1,2) corresponds to the envelope of the electromagnetic radiation passing through the optical fibre and i is the imaginary unit. In the above equation, g 11 and g 22 correspond to the Self Phase Modulation (SPM) while g 12 and g 21 represent the Cross Phase Modulation (XPM). Equations.…”
Section: Introductionmentioning
confidence: 99%