Search results for "Rogue wave"

showing 6 items of 66 documents

Soliton generation and rogue-wave like behavior through fourth order modulation instability

2010

International audience; We numerically study the dynamics of ultra-broadband wavelength converters based on fourth-order scalar modulation instability. We report the spontaneous emergence of solitons and trapped radiation waves as well as L-shaped associated statistical signatures.

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics]Physics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]Cross-phase modulationScalar (mathematics)02 engineering and technologyRadiation01 natural sciencesInstability010309 optics020210 optoelectronics & photonicsModulationQuantum mechanics0103 physical sciences0202 electrical engineering electronic engineering information engineeringSolitonRogue wavePhotonic-crystal fiber
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Complex rogue wave in the fiber optics

2016

This manuscript presents the generation of complex rogue waves related to nonlinear instabilities occurring through the propagation of light in standard optical fibers. Linear and nonlinear physical phenomena involved are first listed, in particular some of them by analogy with the field of hydrodynamics. The different forms of rogue waves induced by the modulation instability process are then presented. They are also known as "breathers", and they are obtained by solving the nonlinear Schrödinger equation. From these exact solutions, various experimental systems were designed by means of numerical simulations based on two rogue-wave excitation methods. The first one is an exact generation …

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics]Équation de Schrödinger non-linéaireFibres optiquesRogue wavesInstabilité de modulationSystème de ManakovPolarizationNonlinear Schrödinger equationOptique non-linéaire ultrarapideUltrafast nonlinear opticsOptical fibersManakov systemOndes scélératesModulation instabilityPolarisation
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18 parameter deformations of the Peregrine breather of order 10 solutions of the NLS equation

2015

We present here new solutions of the focusing one-dimensional nonlinear Schrödinger (NLS) 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 rings as found for the lower-orders.

[PHYS]Physics [physics]PolynomialBreatherMathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear PhysicsComputer Science ApplicationsExponential functionsymbols.namesakeNonlinear systemComputational Theory and MathematicsProduct (mathematics)symbolsPeregrine solitonRogue wave[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Nonlinear Sciences::Pattern Formation and SolitonsMathematical PhysicsSchrödinger's catComputingMilieux_MISCELLANEOUSMathematics
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8-parameter solutions of fifth order to the Johnson equation

2019

We give different representations of the solutions of the Johnson equation with parameters. First, an expression in terms of Fredholm determinants is given; we give also a representation of the solutions written as a quotient of wronskians of order 2N. These 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 polyno-mials of degree 2N (N +1) in x, t and 4N (N +1) in y depending on 2N −2 parameters. Here, we explicitly construct the expressions of the rational solutions of order 5 depending on 8 real parameters and we study the patterns of their modulus in the plane (x, y) and their …

rogue waves PACS numbers : 33Q55ratio- nal solutionswronskiansrational solutions[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Johnson equation4710A-[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K104735Fg4754BdFredholm determinants
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From first to fourth order rational solutions to the Boussinesq equation

2020

Rational solutions to the Boussinesq equation are constructed as a quotient of two polynomials in x and t. For each positive integer N , the numerator is a polynomial of degree N (N + 1) − 2 in x and t, while the denominator is a polynomial of degree N (N + 1) in x and t. So we obtain a hierarchy of rational solutions depending on an integer N called the order of the solution. We construct explicit expressions of these rational solutions for N = 1 to 4.

rogue waves PACS numbers : 33Q55rational solutions[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]4710A-[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K104735Fg4754BdBoussinesq equation
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First and second order rational solutions to the Johnson equation and rogue waves

2018

Rational solutions to the Johnson equation are constructed as a quotient of two polynomials in x, y and t depending on several real parameters. We obtain an infinite hierarchy of rational solutions written in terms of polynomials of degrees 2N (N + 1) in x, and t, 4N (N + 1) in y, depending on 2N − 2 real parameters for each positive integer N. We construct explicit expressions of the solutions in the cases N = 1 and N = 2 which are given in the following. We study the evolution of the solutions by constructing the patterns of their modulus in the (x, y) plane, and this for different values of parameters.

wronskiansJohnson equation4710A-[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]ratio-rogue wavesnal solutions37K10[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]33Q554735FgPACS numbers :4754BdFredholm determinants
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