Search results for "Mathematical physics"

showing 10 items of 2687 documents

Families of rational solutions to the KPI equation of order 7 depending on 12 parameters

2017

International audience; We construct in this paper, rational solutions as a quotient of two determinants of order 2N = 14 and we obtain what we call solutions of order N = 7 to the Kadomtsev-Petviashvili equation (KPI) as a quotient of 2 polynomials of degree 112 in x, y and t depending on 12 parameters. The maximum of modulus of these solutions at order 7 is equal to 2(2N + 1)2= 450. We make the study of the patterns of their modulus in the plane (x, y) and their evolution according to time and parameters a1, a2, a3, a4, a5, a6, b1, b2, b3, b4, b5, b6. When all these parameters grow, triangle and ring structures are obtained.

KPI equationWronskians[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 determinantsPACS numbers: 33Q55 37K10 47.10A- 47.35.Fg 47.54.Bd
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Rational solutions to the KPI equation of order 7 depending on 12 parameters

2018

We construct in this paper, rational solutions as a quotient of two determinants of order 2N = 14 and we obtain what we call solutions of order N = 7 to the Kadomtsev-Petviashvili equation (KPI) as a quotient of 2 polynomials of degree 112 in x, y and t depending on 12 parameters. The maximum of modulus of these solutions at order 7 is equal to 2(2N + 1) 2 = 450. We make the study of the patterns of their modulus in the plane (x, y) and their evolution according to time and parameters a1, a2, a3, a4, a5, a6, b1, b2, b3, b4, b5, b6. When all these parameters grow, triangle and ring structures are obtained.

KPI equation[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Wronskians[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]rogue waveslumps[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Fredholm determinants
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Rational solutions to the KdV equation depending on multi-parameters

2021

We construct multi-parametric rational solutions to the KdV equation. For this, we use solutions in terms of exponentials depending on several parameters and take a limit when one of these parameters goes to 0. Here we present degenerate rational solutions and give a result without the presence of a limit as a quotient of polynomials depending on 3N parameters. We give the explicit expressions of some of these rational solutions.

KdV equation47.35.Fg47.10A-rational solutions PACS numbers : 33Q55[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]47.54.Bd[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K10
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Degenerate Riemann theta functions, Fredholm and wronskian representations of the solutions to the KdV equation and the degenerate rational case

2021

International audience; We degenerate the finite gap solutions of the KdV equation from the general formulation given in terms of abelian functions when the gaps tend 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.We construct also multi-parametric degenerate rational solutions of this equation.

KdV equationPure mathematicsGeneral Physics and AstronomyFredholm determinantTheta function01 natural sciencessymbols.namesakeWronskians[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Fredholm determinant0103 physical sciencesRiemann theta functions0101 mathematicsAbelian group010306 general physicsKorteweg–de Vries equationMathematical PhysicsMathematicsWronskianRiemann surface010102 general mathematicsDegenerate energy levelsRiemann hypothesisNonlinear Sciences::Exactly Solvable and Integrable SystemsRiemann surfacesymbolsGeometry and Topology
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Khovanov homology for signed divides

2009

The purpose of this paper is to interpret polynomial invariants of strongly invertible links in terms of Khovanov homology theory. To a divide, that is a proper generic immersion of a finite number of copies of the unit interval and circles in a [math] –disc, one can associate a strongly invertible link in the [math] –sphere. This can be generalized to signed divides: divides with [math] or [math] sign assignment to each crossing point. Conversely, to any link [math] that is strongly invertible for an involution [math] , one can associate a signed divide. Two strongly invertible links that are isotopic through an isotopy respecting the involution are called strongly equivalent. Such isotopi…

Khovanov homologyPure mathematicsDivides[ MATH.MATH-AT ] Mathematics [math]/Algebraic Topology [math.AT]Homology (mathematics)01 natural scienceslaw.inventionMorse signed dividessymbols.namesakelawEuler characteristic0103 physical sciencesFOS: MathematicsAlgebraic Topology (math.AT)Mathematics - Algebraic Topology0101 mathematicsInvariant (mathematics)Finite setMathematicsKhovanov homology010102 general mathematics16. Peace & justiceInvertible matrix57M27[MATH.MATH-AT]Mathematics [math]/Algebraic Topology [math.AT]IsotopysymbolsStrongly invertible links010307 mathematical physicsGeometry and TopologyVector space
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Invariant rotational curves in Sitnikov's Problem

1993

The Sitnikov's Problem is a Restricted Three-Body Problem of Celestial Mechanics depending on a parameter, the eccentricity,e. The Hamiltonian,H(z, v, t, e), does not depend ont ife=0 and we have an integrable system; ife is small the KAM Theory proves the existence of invariant rotational curves, IRC. For larger eccentricities, we show that there exist two complementary sequences of intervals of values ofe that accumulate to the maximum admissible value of the eccentricity, 1, and such that, for one of the sequences IRC around a fixed point persist. Moreover, they shrink to the planez=0 ase tends to 1.

Kolmogorov–Arnold–Moser theoremApplied MathematicsMathematical analysisKepler's laws of planetary motionAstronomy and AstrophysicsGeometryInvariant (physics)Fixed pointThree-body problemSitnikov problemCelestial mechanicsComputational Mathematicssymbols.namesakeSpace and Planetary ScienceModeling and SimulationsymbolsAstrophysics::Earth and Planetary AstrophysicsHamiltonian (quantum mechanics)Mathematical PhysicsMathematicsCelestial Mechanics & Dynamical Astronomy
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Nodal Solutions for Supercritical Laplace Equations

2015

In this paper we study radial solutions for the following equation $$\Delta u(x)+f (u(x), |x|) = 0,$$ where $${x \in {\mathbb{R}^{n}}}$$ , n > 2, f is subcritical for r small and u large and supercritical for r large and u small, with respect to the Sobolev critical exponent $${2^{*} = \frac{2n}{n-2}}$$ . The solutions are classified and characterized by their asymptotic behaviour and nodal properties. In an appropriate super-linear setting, we give an asymptotic condition sufficient to guarantee the existence of at least one ground state with fast decay with exactly j zeroes for any j ≥ 0. Under the same assumptions, we also find uncountably many ground states with slow decay, singular gro…

Laplace transform010102 general mathematicsMathematical analysisInvariant manifoldStatistical and Nonlinear Physicsradial solutionLaplace equations radial solutions regular/singular ground state Fowler inversion invariant manifoldLaplace equation01 natural sciencesSupercritical fluidinvariant manifold.010101 applied mathematicsSobolev spaceregular/singular ground stateTransformation (function)Structural stabilityFowler inversion0101 mathematicsGround stateCritical exponentMathematical PhysicsMathematicsMathematical physics
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Zero Viscosity Limit for Analytic Solutions, of the Navier-Stokes Equation on a Half-Space.¶I. Existence for Euler and Prandtl Equations

1998

This is the first of two papers on the zero-viscosity limit for the incompressible Navier-Stokes equations in a half-space. In this paper we prove short time existence theorems for the Euler and Prandtl equations with analytic initial data in either two or three spatial dimensions. The main technical tool in this analysis is the abstract Cauchy-Kowalewski theorem. For the Euler equations, the projection method is used in the primitive variables, to which the Cauchy-Kowalewski theorem is directly applicable. For the Prandtl equations, Cauchy-Kowalewski is applicable once the diffusion operator in the vertical direction is inverted.

Laplace's equationIndependent equationSemi-implicit Euler methodPrandtl numberMathematical analysisMathematics::Analysis of PDEsStatistical and Nonlinear PhysicsBackward Euler methodEuler equationsPhysics::Fluid DynamicsEuler methodsymbols.namesakeEuler's formulasymbolsMathematical PhysicsMathematicsCommunications in Mathematical Physics
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Zero Viscosity Limit for Analytic Solutions of the Navier-Stokes Equation on a Half-Space.¶ II. Construction of the Navier-Stokes Solution

1998

This is the second of two papers on the zero-viscosity limit for the incompressible Navier-Stokes equations in a half-space in either 2D or 3D. Under the assumption of analytic initial data, we construct solutions of Navier-Stokes for a short time which is independent of the viscosity. The Navier-Stokes solution is constructed through a composite asymptotic expansion involving the solutions of the Euler and Prandtl equations, which were constructed in the first paper, plus an error term. This shows that the Navier-Stokes solution goes to an Euler solution outside a boundary layer and to a solution of the Prandtl equations within the boundary layer. The error term is written as a sum of firs…

Laplace's equationPrandtl numberMathematical analysisMathematics::Analysis of PDEsCharacteristic equationStatistical and Nonlinear PhysicsStokes flowPhysics::Fluid Dynamicssymbols.namesakeBoundary layerNonlinear systemStokes' lawEuler's formulasymbolsMathematical PhysicsMathematicsCommunications in Mathematical Physics
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An FPGA based Topological Processor Prototype for the ATLAS Level-1 Trigger Upgrade

2012

By 2014 the LHC will collide proton bunches at 14TeV with an increased instantaneous luminosity up to 3·10³⁴cm⁻²s⁻¹. The resulting higher event rate will challenge the existing ATLAS trigger system. A reduction on the trigger rate can be achieved by selecting interesting channels based on their expected decay topology and thus reducing background. This will be achieved by introducing of a new FPGA based module in the Level-1 trigger: the Topological Processor L1Topo. With L1Topo it will be possible for the first time to concentrate detailed information from the entire calorimeters and the muon detector into a single module. L1Topo will receive a total aggregate bandwidth of 1Tb/s. The data …

Large Hadron ColliderBandwidth (signal processing)TopologyLinear particle acceleratorComputer Science::Hardware ArchitectureData acquisitionBunchesUpgradePhysics::Accelerator PhysicsTransceiverDetectors and Experimental TechniquesField-programmable gate arrayInstrumentationMathematical Physics
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