Search results for "Integrable systems"

showing 10 items of 256 documents

Riemann theta functions, Fredholm and wronskian representations of the solutions to the KdV equation

2021

We degenerate the finite gap solutions of the KdV equation from the general formulation given in terms of abelian functions when the gaps tends to points, to get solutions to the KdV equation given in terms of Fredholm determinants and wronskians. For this we establish a link between Riemann theta functions, Fredholm determinants and wronskians. This gives the bridge between the algebro-geometric approach and the Darboux dressing method.

Nonlinear Sciences::Exactly Solvable and Integrable Systems[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Mathematics::Spectral Theory
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2N+1 highest amplitude of the modulus of the N-th order AP breather and other 2N-2 parameters solutions to the NLS equation

2015

We construct here new deformations of the AP breather (Akhmediev-Peregrine breather) of order N (or AP N breather) with 2N −2 real parameters. Other families of quasi-rational solutions of the NLS equation are obtained. We evaluate the highest amplitude of the modulus of AP breather of order N ; we give the proof that the highest amplitude of the AP N breather is equal to 2N + 1. We get new formulas for the solutions of the NLS equation, different from these already given in previous works. New solutions for the order 8 and their deformations according to the parameters are explicitly given. We get the triangular configurations as well as isolated rings at the same time. Moreover, the appea…

Nonlinear Sciences::Exactly Solvable and Integrable Systemsnumbers : 33Q55[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]4710A-[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]37K10[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]4754Bd 1Nonlinear Sciences::Pattern Formation and Solitons33Q55 37K10 47.10A- 47.35.Fg 47.54.Bd4735Fg
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Families of solutions to the CKP equation with multi-parameters

2020

We construct solutions to the CKP (cylindrical Kadomtsev-Petviashvili)) equation in terms of Fredholm determinants. We deduce solutions written as a quotient of wronskians of order 2N. These solutions are called solutions of order N ; they depend on 2N − 1 parameters. They can be written as a quotient of 2 polynomials of degree 2N (N + 1) in x, t and 4N (N + 1) in y depending on 2N − 2 parameters. We explicitly construct the expressions up to order 5 and we study the patterns of their modulus in plane (x, y) and their evolution according to time and parameters.

Nonlinear Sciences::Exactly Solvable and Integrable Systemswronskiansrational solutions[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]4710A-[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph][MATH.MATH-AP] Mathematics [math]/Analysis of PDEs [math.AP]37K10CKP equation PACS numbers : 33Q554735Fg4754BdFredholm determinants
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Measurement of the top quark mass in the dilepton channel

2007

We present a measurement of the top quark mass in the dilepton channel based on approximately 370/pb of data collected by the D0 experiment during Run II of the Fermilab Tevatron collider. We employ two different methods to extract the top quark mass. We show that both methods yield consistent results using ensemble tests of events generated with the D0 Monte Carlo simulation. We combine the results from the two methods to obtain a top quark mass m_t = 178.1 +/- 8.2 GeV. The statistical uncertainty is 6.7 GeV and the systematic uncertainty is 4.8 GeV.

Nuclear and High Energy PhysicsParticle physicsTop quarkMonte Carlo methodTevatronFOS: Physical sciences01 natural sciencesBottom quarkHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Atomic and Molecular ClustersFermilab010306 general physicsColliderNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyD0 experimentNonlinear Sciences::Exactly Solvable and Integrable SystemsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCommunication channel
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Thermodynamics of Toda lattice models: application to DNA

1993

Abstract Our generalised Bethe ansatz method is used to formulate the statistical mechanics of the classical Toda lattice in terms of a set of coupled integral equations expressed in terms of appropriate action-angle variables. The phase space as coordinatised by these action-angle variables is constrained; and both the soliton number density and the soliton contribution to the free energy density can be shown to decouple from the phonon degrees of freedom and to depend only on soliton-soliton interactions. This makes it possible to evaluate the temperature dependence of the soliton number density which, to leading order, is found to be proportional to T 1 3 .

Number densityDegrees of freedom (physics and chemistry)Statistical and Nonlinear PhysicsStatistical mechanicsCondensed Matter PhysicsBethe ansatzNonlinear Sciences::Exactly Solvable and Integrable SystemsPhase spaceSolitonPerturbation theory (quantum mechanics)Toda latticeNonlinear Sciences::Pattern Formation and SolitonsMathematicsMathematical physicsPhysica D: Nonlinear Phenomena
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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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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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Peregrine soliton generation and breakup in standard telecommunications fiber

2011

International audience; We present experimental and numerical results showing the generation and breakup of the Peregrine soliton in standard telecommunications fiber. The impact of non-ideal initial conditions is studied through direct cut back measurements of the longitudinal evolution of the emerging soliton dynamics, and is shown to be associated with the splitting of the Peregrine soliton into two subpulses, with each subpulse itself exhibiting Peregrine soliton characteristics. Experimental results are in good agreement with simulations.

Optical fiberSoliton (optics)01 natural scienceslaw.invention010309 opticssymbols.namesakeOpticsBrillouin scatteringlaw0103 physical sciencesFiber010306 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]Computer simulationbusiness.industryBreakupAtomic and Molecular Physics and OpticsNonlinear Sciences::Exactly Solvable and Integrable SystemssymbolsPeregrine solitonbusinessTelecommunicationsRaman scattering
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"Table 2" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Detailed list of the contribution of each source of uncertainty to the total uncertainty on the measured values of $\sigma(tq)$, $\sigma(\bar{t}q)$, $R_t$, and $\sigma(tq+\bar{t}q)$. The evaluation of the systematic uncertainties has a statistical uncertainty of $0.3\,\%$. Uncertainties contributing less than $1.0\,\%$ are marked with "$<1$" in the paper. To provide numerical values for this table in HEPdata, these uncertainties are approximated with $\pm 0.5\,\%$. This approximation is applied to all measurements for the following uncertainties$:$ JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by-jets, JES pileup, $b$-JES, jet vertex fraction, mistag e…

P P --> TOP XHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySystematic uncertaintiesTop7000.0SIGComputer Science::Computers and SocietyInclusiveSingle Differential Cross SectionP P --> TOPBAR XNonlinear Sciences::Exactly Solvable and Integrable SystemsTotal cross sectionProton-Proton ScatteringPhysics::Atomic and Molecular Clusterst-channel productionDSIG/DPTHigh Energy Physics::ExperimentTransverse Momentum Dependence
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"Table 4" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Parametrization factors for the $m_{t}$ dependence [see Eq. (4) in the paper] of $\sigma(tq)$, $\sigma(\bar tq)$, and $\sigma(t q+\bar t q)$.

P P --> TOP XHigh Energy Physics::LatticeRapidity DependenceHigh Energy Physics::PhenomenologyTop7000.0DSIG/DYRAPSIGSingle Differential Cross SectionP P --> TOPBAR XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsTotal cross-sectionProton-Proton ScatteringPhysics::Atomic and Molecular ClustersHigh Energy Physics::Experiment
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