Search results for "SOLITON"

showing 10 items of 534 documents

Interacting Solitons in a High Index Glass

2010

We investigate the interaction of two coherent 2D+1 solitary beams in a high index glass.

PhysicsIndex (economics)OpticsKerr effectOptical glassCondensed matter physicsbusiness.industryNonlinear opticsbusinessRefractive indexWaveguide (optics)Nonlinear optics Kerr effect Spatial solitonsConference on Lasers and Electro-Optics 2010
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Analog simulation of neural information propagation using an electrical FitzHugh-Nagumo lattice

2004

International audience; A nonlinear electrical lattice modelling neural information propagation is presented. It is shown that our system is an analog simulator of the FitzHugh-Nagumo equations, and hence supports pulse propagation with the appropriate properties.

PhysicsInformation propagationQuantitative Biology::Neurons and CognitionGeneral MathematicsApplied MathematicsQuantitative Biology::Tissues and OrgansGeneral Physics and AstronomyStatistical and Nonlinear PhysicsFitzhugh nagumo01 natural sciences010305 fluids & plasmasPulse propagationNonlinear system[NLIN.NLIN-PS]Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]Lattice (order)0103 physical sciences[ NLIN.NLIN-PS ] Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]Statistical physicsFitzHugh–Nagumo model010306 general physicsNonlinear Sciences::Pattern Formation and Solitons
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Soliton collisions with shape change by intensity redistribution in mixed coupled nonlinear Schrodinger equations

2006

International audience; A different kind of shape changing (intensity redistribution) collision with potential application to signal amplification is identified in the integrable N-coupled nonlinear Schrodinger (CNLS) equations with mixed signs of focusing- and defocusing-type nonlinearity coefficients. The corresponding soliton solutions for the N=2 case are obtained by using Hirota's bilinearization method. The distinguishing feature of the mixed sign CNLS equations is that the soliton solutions can both be singular and regular. Although the general soliton solution admits singularities we present parametric conditions for which nonsingular soliton propagation can occur. The multisoliton …

PhysicsIntegrable systemSchrödinger equationsymbols.namesakeNonlinear systemDissipative solitonClassical mechanicsNonlinear Sciences::Exactly Solvable and Integrable Systems[ PHYS.PHYS.PHYS-AO-PH ] Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]symbolsPeregrine solitonGravitational singularitySolitonNonlinear Sciences::Pattern Formation and SolitonsSign (mathematics)
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Observation of collapse arrest in pure kerr media sustained by a parametric interaction

2013

We demonstrate a parametric interaction based on four wave mixing that can arrest the collapse and stabilize solitary propagation in a pure Kerr material by controlling the wavelength of the interacting beams.

PhysicsKerr effectCollapse (topology)Physics::OpticsCollapse arrestSettore ING-INF/01 - ElettronicaSolitary propagationWavelengthFour-wave mixingKerr mediaParametric interactionsQuantum electrodynamicsQuantum mechanicsKerr materialsLight beamNonlinear OpticsPhase velocityRefractive indexNonlinear Sciences::Pattern Formation and SolitonsParametric statistics
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Optical kerr effect in the strong field regime

2013

The optical Kerr response of hydrogen atom submitted to a strong and short near infrared laser pulse excitation is studied by solving the full 3D time-dependent Schro¨dinger equation. The nonlinear polarization evaluated at the driving field frequency is compared to the canonical expression derived from perturbation theory. A discrepancy between the two models is observed at large intensity affecting the nonlinear propagation of short and intense laser pulses.

PhysicsKerr effectMagneto-optic Kerr effectMode-lockingQuantum mechanicsCross-phase modulationFilament propagationOptical polarizationSoliton (optics)Physics::Atomic PhysicsAtomic physicsQ-switching
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Switching Dynamics of Dark Solitons in Kerr Microresonators

2019

Dissipative Kerr solitons (DKS) are localized structures in optical resonators that arise from a double balance between dispersion and Kerr effect, and linear loss and parametric gain [1]. The periodic nature of DKS corresponds to frequency combs. DKS can be generated in high-Q microresonators for diverse applications, from coherent communications to precision frequency synthesis [1]. Most studies of DKS have focused on microresonator cavities operating in the anomalous dispersion regime, where the waveforms correspond to bright soliton pulses. Coherent microresonator combs can also be formed in the normal dispersion regime [2]. The time-domain waveform corresponds to a localized dark-pulse…

PhysicsKerr effectOther Electrical Engineering Electronic Engineering Information EngineeringCondensed matter physicsOther Physics TopicsAtom and Molecular Physics and OpticsDynamics (mechanics)Physics::Optics02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesPulse (physics)010309 opticsResonator0103 physical sciencesDispersion (optics)Dissipative systemWaveformSoliton0210 nano-technologyNonlinear Sciences::Pattern Formation and Solitons
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Dynamics of the transition from polarization disorder to antiphase polarization domains in vector fiber lasers

2014

We demonstrate that nonlinear polarization coupling in a fiber ring laser without polarization-selective elements, subject to the effects of average anomalous dispersion, Kerr effect, and nonlinear gain saturation, can lead to the antisynchronization of spatiotemporal chaos into a wide variety of ordered laminar states of orthogonal polarization temporal domains. These antiphase polarization domains include stable lattices of soliton trains with high duty cycle at repetition rates of hundreds of MHz, as well as sparse trains of coupled dark and bright solitary waves.

PhysicsKerr effectPolarization rotatorring lasersCondensed matter physicsOrthogonal polarization spectral imagingbusiness.industryRing laserLaminar flowFiber lasers; ring lasers; solitonsPolarization (waves)Atomic and Molecular Physics and OpticsFiber lasersOpticsDuty cycleFiber lasersolitonsbusiness
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Vectorial Kerr-cavity solitons.

2000

It is shown that a Kerr cavity with different losses for the two polarization components of the field can support both dark and bright cavity solitons (CS’s). A parametrically driven Ginzburg–Landau equation is shown to describe the system for large-cavity anisotropy. In one transverse dimension the nonlinear dynamics of the bright CS’s is numerically investigated.

PhysicsKerr effectbusiness.industryNumerical analysisPhysics::OpticsAstrophysics::Cosmology and Extragalactic AstrophysicsPolarization (waves)Atomic and Molecular Physics and OpticsNonlinear systemOpticsLight propagationPhysics::Accelerator PhysicsTransverse dimensionbusinessAnisotropyNonlinear Sciences::Pattern Formation and SolitonsOptics letters
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Long-range effects on the periodic deformable sine-Gordon chains

1999

The model of long-range interatomic interactions is found to reveal a number of new features, closely connected with the substrate potential shape parameter s. The phase trajectories, as well as an analytical analysis, provide information on a disintegration of solitons upon reaching some critical values of the lattice parameters. An implicit form for two classes of these topological solitons (kink) is calculated exactly.

PhysicsLattice dynamicsLattice (order)General Materials ScienceStatistical physicsSineSolitonCondensed Matter PhysicsCritical valueNonlinear Sciences::Pattern Formation and SolitonsShape parameterJournal of Physics: Condensed Matter
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Numerical study of a multiscale expansion of the Korteweg de Vries equation and Painlev\'e-II equation

2007

The Cauchy problem for the Korteweg de Vries (KdV) equation with small dispersion of order $\e^2$, $\e\ll 1$, is characterized by the appearance of a zone of rapid modulated oscillations. These oscillations are approximately described by the elliptic solution of KdV where the amplitude, wave-number and frequency are not constant but evolve according to the Whitham equations. Whereas the difference between the KdV and the asymptotic solution decreases as $\epsilon$ in the interior of the Whitham oscillatory zone, it is known to be only of order $\epsilon^{1/3}$ near the leading edge of this zone. To obtain a more accurate description near the leading edge of the oscillatory zone we present a…

PhysicsLeading edgeSmall dispersion limitComputer Science::Information RetrievalGeneral MathematicsMathematical analysisGeneral EngineeringMathematics::Analysis of PDEsGeneral Physics and AstronomyNonlinear equationsDispersive partial differential equationShock wavesAmplitudeNonlinear Sciences::Exactly Solvable and Integrable SystemsInitial value problemWavenumberDispersive shockDispersion (water waves)Constant (mathematics)Korteweg–de Vries equationDevries equationAsymptoticsSettore MAT/07 - Fisica MatematicaNonlinear Sciences::Pattern Formation and SolitonsMathematical Physics
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