Search results for "CTL"

showing 10 items of 521 documents

A new proof of the existence of hierarchies of Poisson-Nijenhuis structures

2004

Given a Poisson-Nijenhuis manifold, a two-parameter family of Poisson- Nijenhuis structures can be defined. As a consequence we obtain a new and noninductive proof of the existence of hierarchies of Poisson-Nijenhuis structures.

Nonlinear Sciences::Exactly Solvable and Integrable SystemsMathematics::Differential GeometryMathematics::Symplectic GeometryMatemàtica
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Quantum and Classical Statistical Mechanics of the Integrable Models in 1 + 1 Dimensions

1990

In a short but remarkable paper Yang and Yang [1] showed that the free energy of a model system consisting of N bosons on a line with repulsive δ-function interactions was given by a set of coupled integral equations. The Yangs’ chosen model is in fact the repulsive version of the quantum Nonlinear Schrodinger (NLS) model. We have shown that with appropriate extensions and different dispersion relations and phase shifts similar formulae apply to ‘all’ of the integrable models quantum or classical. These models include the sine-Gordon (s-G) and sinh-Gordon (sinh-G) models, the two NLS models (attractive and repulsive), the Landau-Lifshitz (L-L’) model which includes all four previous models,…

Nonlinear Sciences::Exactly Solvable and Integrable SystemsMethod of quantum characteristicsStatistical mechanicsQuantum inverse scattering methodToda latticeQuantum statistical mechanicsClassical limitQuantum chaosMathematical physicsMathematicsBethe ansatz
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Propagation and Stability of Novel Parametric Interaction Solitons

2006

International audience; We present a new multi-parameter family of analytical soliton solutions for nonlinear three-wave resonant interactions. We show the amplitude, phase-front shapes and general properties of the solitons. The stability of these novel parametric solitons is simply related to the value of their common group velocity.

Nonlinear Sciences::Exactly Solvable and Integrable SystemsNonlinear Sciences::Pattern Formation and Solitons
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"Table 2" of "Measurement of the t anti-t production cross-section in p anti-p collisions using dilepton events"

2008

TOP TOPBAR production cross section for the current Tevatron average top quark mass 170.9 GeV.. Error contains both statistics and systematics.

Nonlinear Sciences::Exactly Solvable and Integrable SystemsPBAR P --> TOP TOPBARHigh Energy Physics::PhenomenologyIntegrated Cross SectionPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentCross SectionSIG1960.0Computer Science::Computers and Society
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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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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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