Search results for "Rogue wave"

showing 10 items of 66 documents

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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Families of solutions of order nine to the NLS equation with sixteen parameters

2015

We construct new deformations of the Peregrine breather (P9) of order 9 with 16 real parameters. With this method, we obtain explicitly new families of quasi-rational solutions to the NLS equation in terms of a product of an exponential depending on t by a ratio of two polynomials of degree 90 in x and t; when all the parameters are equal to 0, we recover the classical P9 breather. We construct new patterns of different types of rogue waves as triangular configurations of 45 peaks as well as rings and concentric rings.

NLS equationPeregrine breather[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]35Q55 37K10.[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences::Pattern Formation and Solitonsrogue waves 1
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Patterns of deformations of P 3 and P 4 breathers solutions to the NLS equation

2016

In this article, one gives a classification of the solutions to the one dimensional nonlinear focusing Schrödinger equation (NLS) by considering the modulus of the solutions in the (x, t) plan in the cases of orders 3 and 4. For this, we use a representation of solutions to NLS equation as a quotient of two determinants by an exponential depending on t. This formulation gives in the case of the order 3 and 4, solutions with respectively 4 and 6 parameters. With this method, beside Peregrine breathers, we construct all characteristic patterns for the modulus of solutions, like triangular configurations, ring and others.

NLS equationPeregrine breather[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue waves[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]
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Tenth Peregrine breather solution of the NLS equation.

2012

We go on in this paper, in the study of the solutions of the focusing NLS equation. With a new representation given in a preceding paper, a very compact formulation without limit as a quotient of two determinants, we construct the Peregrine breather of order N=10. The explicit analytical expression of the Akhmediev's solution is completely given.

NLS equation[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]WronskiansPeregrine breathersRogue waves[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Fredhom determinantsPeregrine breathers.[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Nonlinear Sciences::Pattern Formation and Solitons
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Tenth order solutions to the NLS equation with eighteen parameters

2015

We present here new solutions of the focusing one dimensional non linear Schrödinger equation which appear as deformations of the Peregrine breather of order 10 with 18 real parameters. With this method, we obtain new families of quasi-rational solutions of the NLS equation, and we obtain explicit quotients of polynomial of degree 110 in x and t by a product of an exponential depending on t. We construct new patterns of different types of rogue waves and recover the triangular configurations as well as rings and concentric as found for the lower orders.

NLS equationwronskiansPeregrine breather[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue waves[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]
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Fredholm representations of solutions to the KPI equation, their wronkian versions and rogue waves

2016

We construct solutions to the Kadomtsev-Petviashvili equation (KPI) in terms of Fredholm determinants. We deduce solutions written as a quotient of wronskians of order 2N. These solutions called solutions of order N depend on 2N − 1 parameters. When one of these parameters tends to zero, we obtain N order rational solutions expressed as a quotient of two polynomials of degree 2N (N + 1) in x, y and t depending on 2N − 2 parameters. So we get with this method an infinite hierarchy of solutions to the KPI equation.

Nonlinear Sciences::Exactly Solvable and Integrable Systems[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 determinants
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The Peregrine soliton in nonlinear fibre optics

2010

International audience; The Peregrine soliton is a localized nonlinear structure predicted to exist over 25 years ago, but not so far experimentally observed in any physical system. It is of fundamental significance because it is localized in both time and space, and because it defines the limit of a wide class of solutions to the nonlinear Schrödinger equation (NLSE). Here, we use an analytic description of NLSE breather propagation to implement experiments in optical fibre generating femtosecond pulses with strong temporal and spatial localization, and near-ideal temporal Peregrine soliton characteristics. In showing that Peregrine soliton characteristics appear with initial conditions th…

Optical fiberGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmaslaw.inventionOpticsNonlinear fibre optics[NLIN.NLIN-PS]Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]law0103 physical sciences[ NLIN.NLIN-PS ] Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]Rogue wave010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsPhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]Spacetimebusiness.industryOptical physicsOptical rogue wavesClassical mechanicsNonlinear Sciences::Exactly Solvable and Integrable SystemsFemtosecondPeregrine solitonbusiness
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Shallow water rogue wavetrains in nonlinear optical fibers

2013

International audience; In addition to deep-water rogue waves which develop from the modulation instability of an optical CW, wave propagation in optical fibers may also produce shallow water rogue waves. These extreme wave events are generated in the modulationally stable normal dispersion regime. A suitable phase or frequency modulation of a CW laser leads to chirp-free and flat-top pulses or flaticons which exhibit a stable self-similar evolution. Upon collision, flaticons at different carrier frequencies, which may also occur in wavelength division multiplexed transmission systems, merge into a single, high-intensity, temporally and spatially localized rogue pulse.

Optical fiberNonlinear opticsWave propagationGeneral Physics and AstronomyFOS: Physical sciencesPhysics::Optics02 engineering and technologyPattern Formation and Solitons (nlin.PS)Fluid Mechanics01 natural sciencesInstabilitylaw.invention020210 optoelectronics & photonicsOpticslaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringRogue waveFluid mechanics; nonlinear optics; optical fibers010306 general physicsPhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryRogue wavesOptical fibersFluid Dynamics (physics.flu-dyn)Physics - Fluid DynamicsNonlinear Sciences - Pattern Formation and SolitonsWaves and shallow waterWavelengthPhase modulationbusinessPhase modulationFrequency modulationPhysics - OpticsOptics (physics.optics)
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Polarization modulation instability in a Manakov fiber system

2015

International audience; The Manakov model is the simplest multicomponent model of nonlinear wave theory: It describes elementary stable soliton propagation and multisoliton solutions, and it applies to nonlinear optics, hydrodynamics, and Bose-Einstein condensates. It is also of fundamental interest as an asymptotic model in the context of the widely used wavelength-division-multiplexed optical fiber transmission systems. However, although its physical relevance was confirmed by the experimental observation of Manakov (vector) solitons in a planar waveguide in 1996, there have in fact been no quantitative experiments confirming its validity for nonlinear dynamics other than soliton formatio…

Optical fiberPhysics::OpticsContext (language use)02 engineering and technology01 natural sciencesWaveguide (optics)law.invention020210 optoelectronics & photonics[NLIN.NLIN-PS]Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]law0103 physical sciences0202 electrical engineering electronic engineering information engineeringrandomly varying birefringence; cross-phase modulation; optical-fibers; normal-dispersion; copropagating frequencies; Schrodinger-equations; WDM transmission; rogue waves; generation; solitonRogue wave010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsPhysicsRandomly varying birefringence[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Nonlinear opticsAtomic and Molecular Physics and Opticsoptical-fibersNonlinear systemClassical mechanicsNonlinear Sciences::Exactly Solvable and Integrable Systemscross-phase modulationManakov systemRandomly varying birefringence; cross-phase modulation; optical-fibersSoliton
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