2015
DOI: 10.5890/jand.2015.06.001
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Study of the Effect of the Coupling in a Dispersion-managed Dual Core Optical Fiber Using the Collective Variables Approach

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Cited by 3 publications
(2 citation statements)
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“…It is to be noted that the simulations are made for input asymmetric parameters as follows; u 10 = 1, v 10 = 0.75 and u 30 = v 30 = 1. Let us remember the dimensionless transformation [51]; x = X LD , and L D = T 2 0 |β2| ; X being the real distance, L D the dispersion length, T 0 the width of the pulse and β 2 the GVD coefficient (related to p r through the relation p r = β2 2 ). We adopt the physical parameters corresponding to standard nonlinear directional couplers, as follows [22]: β 2 = 0.02ps 2 /m, T 0 = 50f s at λ = 1.5µm.…”
Section: Energy Ratiomentioning
confidence: 99%
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“…It is to be noted that the simulations are made for input asymmetric parameters as follows; u 10 = 1, v 10 = 0.75 and u 30 = v 30 = 1. Let us remember the dimensionless transformation [51]; x = X LD , and L D = T 2 0 |β2| ; X being the real distance, L D the dispersion length, T 0 the width of the pulse and β 2 the GVD coefficient (related to p r through the relation p r = β2 2 ). We adopt the physical parameters corresponding to standard nonlinear directional couplers, as follows [22]: β 2 = 0.02ps 2 /m, T 0 = 50f s at λ = 1.5µm.…”
Section: Energy Ratiomentioning
confidence: 99%
“…Recently, we have highlighted the interaction between two Gaussian pulses propagating in such a fiber laser by the means of collective variables approach [51]. This interaction was governed by a pair of CQ-CGLE without higher order dispersion (HOD) terms.…”
Section: Introductionmentioning
confidence: 99%