Search results for "Rogue waves"

showing 10 items of 35 documents

Roadmap on optical rogue waves and extreme events

2016

Nail Akhmediev et al. ; 38 págs.; 28 figs.

:Ciències de la visió::Òptica física [Àrees temàtiques de la UPC]extreme eventsNonlinear opticsFreak-wavesProcess (engineering)Subject (philosophy)Supercontinuum generationPeregrine soliton01 natural sciences010309 opticsOptics0103 physical sciencesZero-dispersion wavelength[NLIN]Nonlinear Sciences [physics]Rogue wave010306 general physicsModulation instabilityComputingMilieux_MISCELLANEOUSPhysicsÒptica no lineal:Física [Àrees temàtiques de la UPC]Nonlinear schrodinger-equationbusiness.industryGinzburg-Landau equationnonlinear opticsRogue wavesOptical rogue wavesrogue wavesextreme events; nonlinear optics; rogue wavesExtreme eventsValue statisticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsVariety (cybernetics)Photonic crystal fibersWork (electrical)Noise-like pulsesPeregrine solitonbusinessScientific terminology
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Ondes scélérates et statistiques extrêmes dans les systèmes optiques fibrés

2011

This thesis deals with extremes statistics which has become an attractive subject in optics since a comparison with oceanic rogue waves has been proposed at the end of 2007. We report some potential mechanisms stimulating the rogue wave formation in the context of guided propagation of light in optical fibers. In a first part, we explore optical rogue waves in supercontinuums generated by fourth-order modulation instability and we propose a stabilization method based on the use of two continuous seeds. Then, we present a detailed study on Raman fiber amplifiers where we determine the conditions of emergence of giant structures : in presence of a partially incoherent pumping wave, a quasi-in…

Amplificateur RamanOptical fiberNonlinear opticsRogue waves[ PHYS.COND.CM-GEN ] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Raman amplifierExtreme statisticsFibre optiqueStatistiques extrêmesOptique non-linéaire[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other][PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]SolitonOndes scélérates
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Dissipative rogue wave generation in multiple-pulsing mode-locked fiber laser

2013

Following the first experimental observation of a new mechanism leading to optical rogue wave (RW) formation briefly reported in Lecaplain et al (2012 Phys. Rev. Lett. 108 233901), we provide an extensive study of the experimental conditions under which these RWs can be detected. RWs originate from the nonlinear interactions of bunched chaotic pulses that propagate in a fiber laser cavity, and manifest as rare events of high optical intensity. The crucial influence of the electrical detection bandwidth is illustrated. We also clarify the observation of RWs with respect to other pulsating regimes, such as Q-switching instability, that also lead to L-shaped probability distribution functions.…

Dissipative systemChaoticPhysics::OpticsSolitonsInstabilitylaw.inventionOpticslawFiber laserRogue waveOptical rogue wavesExtreme eventPhysicsbusiness.industryFiber laserOptical rogue wavesDissipative solitonsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsNonlinear systemNonlinear dynamicsOptical cavityMode-locked laserDissipative systemChaosbusinessJournal of Optics
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Families of rational solutions to the KPI equation of order 7 depending on 12 parameters

2017

International audience; We construct in this paper, rational solutions as a quotient of two determinants of order 2N = 14 and we obtain what we call solutions of order N = 7 to the Kadomtsev-Petviashvili equation (KPI) as a quotient of 2 polynomials of degree 112 in x, y and t depending on 12 parameters. The maximum of modulus of these solutions at order 7 is equal to 2(2N + 1)2= 450. We make the study of the patterns of their modulus in the plane (x, y) and their evolution according to time and parameters a1, a2, a3, a4, a5, a6, b1, b2, b3, b4, b5, b6. When all these parameters grow, triangle and ring structures are obtained.

KPI equationWronskians[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Rogue waves[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]LumpsFredholm determinantsPACS numbers: 33Q55 37K10 47.10A- 47.35.Fg 47.54.Bd
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Rational solutions to the KPI equation of order 7 depending on 12 parameters

2018

We construct in this paper, rational solutions as a quotient of two determinants of order 2N = 14 and we obtain what we call solutions of order N = 7 to the Kadomtsev-Petviashvili equation (KPI) as a quotient of 2 polynomials of degree 112 in x, y and t depending on 12 parameters. The maximum of modulus of these solutions at order 7 is equal to 2(2N + 1) 2 = 450. We make the study of the patterns of their modulus in the plane (x, y) and their evolution according to time and parameters a1, a2, a3, a4, a5, a6, b1, b2, b3, b4, b5, b6. When all these parameters grow, triangle and ring structures are obtained.

KPI equation[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Wronskians[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue waveslumps[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Fredholm determinants
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Higher order Peregrine breathers solutions to the NLS equation

2015

The solutions to the one dimensional focusing nonlinear Schrödinger equation (NLS) can be written as a product of an exponential depending on t by a quotient of two polynomials of degree N (N + 1) in x and t. These solutions depend on 2N − 2 parameters : when all these parameters are equal to 0, we obtain the famous Peregrine breathers which we call PN breathers. Between all quasi-rational solutions of the rank N fixed by the condition that its absolute value tends to 1 at infinity and its highest maximum is located at the point (x = 0, t = 0), the PN breather is distinguished by the fact that PN (0, 0) = 2N + 1. We construct Peregrine breathers of the rank N explicitly for N ≤ 11. We give …

NLS equationHistoryDegree (graph theory)BreatherPeregrine breathersMathematical analysis[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue wavesAbsolute value (algebra)Rank (differential topology)Computer Science ApplicationsEducationExponential functionsymbols.namesake[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]symbolsOrder (group theory)[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]PACS numbers : 33Q55 37K10 47.10A- 47.35.Fg 47.54.BdNonlinear Schrödinger equationQuotientMathematicsMathematical physicsJournal of Physics: Conference Series
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Hierarchy of solutions to the NLS equation and multi-rogue waves.

2014

The solutions to the one dimensional focusing nonlinear Schrödinger equation (NLS) are given in terms of determinants. The orders of these determinants are arbitrarily equal to 2N for any nonnegative integer $N$ and generate a hierarchy of solutions which can be written as a product of an exponential depending on t by a quotient of two polynomials of degree N(N+1) in x and t. These solutions depend on 2N-2 parameters and can be seen as deformations with 2N-2 parameters of the Peregrine breather P_{N} : when all these parameters are equal to 0, we recover the P_{N} breather whose the maximum of the module is equal to 2N+1. Several conjectures about the structure of the solutions are given.

NLS equationHistorywronskiansDegree (graph theory)Breatherrogue waves.Mathematical analysisPeregrine breathers[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue waves33Q55 37K10 47.10A- 47.35.Fg 47.54.BdComputer Science ApplicationsEducationExponential functionsymbols.namesakeInteger[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Product (mathematics)symbols[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Rogue waveNonlinear Schrödinger equationQuotientMathematics
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Families of deformations of the thirteen peregrine breather solutions to the NLS equation depending on twenty four parameters

2017

International audience; We go on with the study of the solutions to the focusing one dimensional nonlinear Schrodinger equation (NLS). We construct here the thirteen's Peregrine breather (P13 breather) with its twenty four real parameters, creating deformation solutions to the NLS equation. New families of quasirational solutions to the NLS equation in terms of explicit ratios of polynomials of degree 182 in x and t multiplied by an exponential depending on t are obtained. We present characteristic patterns of the modulus of these solutions in the (x; t) plane, in function of the different parameters.

NLS equationNonlinear Sciences::Exactly Solvable and Integrable SystemsPeregrine breather[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]MSC: 35Q55 37K10Rogue waves[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences::Pattern Formation and Solitons
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Degenerate determinant representation of solutions of the NLS equation, higher Peregrine breathers and multi-rogue waves.

2012

We present a new representation of solutions of the focusing NLS equation as a quotient of two determinants. This work is based on a recent paper in which we have constructed a multi-parametric family of this equation in terms of wronskians. This formulation was written in terms of a limit involving a parameter. Here we give a very compact formulation without presence of a limit. This is a completely new result which gives a very efficient procedure to construct families of quasi-rational solutions of the NLS equation. With this method, we construct Peregrine breathers of orders N=4 to 7 and multi-rogue waves associated by deformation of parameters.

NLS equationNonlinear Sciences::Exactly Solvable and Integrable SystemsWronskians[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Peregrine breathersRogue waves[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Riemann theta functions[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences::Pattern Formation and Solitonsfredholm determinantsAkhmediev's breathers
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Solutions to the NLS equation : differential relations and their different representations

2020

Solutions to the focusing nonlinear Schrödinger equation (NLS) of order N depending on 2N − 2 real parameters in terms of wronskians and Fredholm determinants are given. These solutions give families of quasirational solutions to the NLS equation denoted by vN and have been explicitly constructed until order N = 13. These solutions appear as deformations of the Peregrine breather PN as they can be obtained when all parameters are equal to 0. These quasi rational solutions can be expressed as a quotient of two polynomials of degree N (N + 1) in the variables x and t and the maximum of the modulus of the Peregrine breather of order N is equal to 2N + 1. Here we give some relations between sol…

NLS equationNonlinear Sciences::Exactly Solvable and Integrable Systemswronskians[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Peregrine breathersrogue waves[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences::Pattern Formation and SolitonsFredholm determinants
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