Search results for "Hamiltonian system"

showing 10 items of 58 documents

An Interlude: Writing the Hamiltonian

2012

Discrete mathematicssymbols.namesakesymbolsSuperintegrable Hamiltonian systemHamiltonian (quantum mechanics)MathematicsMathematical physicsQuantum Dynamics for Classical Systems
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Massive evaluation and analysis of Poincar�� recurrences on grids of initial data: a tool to map chaotic diffusion

2020

We present a novel numerical method aimed to characterize global behaviour, in particular chaotic diffusion, in dynamical systems. It is based on an analysis of the Poincar\'e recurrence statistics on massive grids of initial data or values of parameters. We concentrate on Hamiltonian systems, featuring the method separately for the cases of bounded and non-bounded phase spaces. The embodiments of the method in each of the cases are specific. We compare the performances of the proposed Poincar\'e recurrence method (PRM) and the custom Lyapunov exponent (LE) methods and show that they expose the global dynamics almost identically. However, a major advantage of the new method over the known g…

Dynamical systems theoryComputer scienceChaoticGeneral Physics and AstronomyFOS: Physical sciencesLyapunov exponent01 natural sciences010305 fluids & plasmasHamiltonian systemsymbols.namesakeSimple (abstract algebra)0103 physical sciencesApplied mathematicsDiffusion (business)010306 general physicsInstrumentation and Methods for Astrophysics (astro-ph.IM)ComputingMilieux_MISCELLANEOUSEarth and Planetary Astrophysics (astro-ph.EP)Numerical analysisNonlinear Sciences - Chaotic DynamicsHardware and ArchitectureBounded functionsymbolsChaotic Dynamics (nlin.CD)Astrophysics - Instrumentation and Methods for Astrophysics[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Astrophysics - Earth and Planetary Astrophysics
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An upper bound of the index of an equilibrium point in the plane

2012

Abstract We give an upper bound of the index of an isolated equilibrium point of a C 1 vector field in the plane. The vector field is decomposed in gradient and Hamiltonian components. This decomposition is related with the Loewner vector field. Associated to this decomposition we consider the set Π where the gradient and Hamiltonian components are linearly dependent. The number of branches of Π starting at the equilibrium point determines the upper bound of the index.

Equilibrium pointApplied MathematicsMathematical analysisGradient systemsUpper and lower boundsIndexsymbols.namesakesymbolsVector fieldLinear independenceHamiltonian systemsHamiltonian (quantum mechanics)AnalysisPlanar differential systemsMathematics
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Some notes on a superlinear second order Hamiltonian system

2016

Variational methods are used in order to establish the existence and the multiplicity of nontrivial periodic solutions of a second order dynamical system. The main results are obtained when the potential satisfies different superquadratic conditions at infinity. The particular case of equations with a concave-convex nonlinear term is covered.

General Mathematicsmedia_common.quotation_subject010102 general mathematicsMathematical analysisPrimary 34C25; Secondary 34B15; Mathematics (all)Algebraic geometryDynamical systemInfinity01 natural sciencesHamiltonian systemTerm (time)010101 applied mathematicsNonlinear systemNumber theorySecondary 34B15Order (group theory)Primary 34C250101 mathematicsMathematicsmedia_common
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Non-equivariant cylindrical contact homology

2013

It was pointed out by Eliashberg in his ICM 2006 plenary talk that the integrable systems of rational Gromov-Witten theory very naturally appear in the rich algebraic formalism of symplectic field theory (SFT). Carefully generalizing the definition of gravitational descendants from Gromov-Witten theory to SFT, one can assign to every contact manifold a Hamiltonian system with symmetries on SFT homology and the question of its integrability arises. While we have shown how the well-known string, dilaton and divisor equations translate from Gromov-Witten theory to SFT, the next step is to show how genus-zero topological recursion translates to SFT. Compatible with the example of SFT of closed …

Geodesic010102 general mathematicsHomology (mathematics)Topology01 natural sciencesHamiltonian system0103 physical sciencesHomogeneous spaceEquivariant mapDilaton010307 mathematical physicsGeometry and Topology0101 mathematicsAlgebraic numberMathematics::Symplectic GeometrySymplectic geometryMathematicsJournal of Symplectic Geometry
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On critical behaviour in systems of Hamiltonian partial differential equations

2013

Abstract We study the critical behaviour of solutions to weakly dispersive Hamiltonian systems considered as perturbations of elliptic and hyperbolic systems of hydrodynamic type with two components. We argue that near the critical point of gradient catastrophe of the dispersionless system, the solutions to a suitable initial value problem for the perturbed equations are approximately described by particular solutions to the Painlevé-I (P $$_I$$ I ) equation or its fourth-order analogue P $$_I^2$$ I 2 . As concrete examples, we discuss nonlinear Schrödinger equations in the semiclassical limit. A numerical study of these cases provides strong evidence in support of the conjecture.

Hamiltonian PDEsFOS: Physical sciencesSemiclassical physicsPainlevé equationsArticleSchrödinger equationHamiltonian systemsymbols.namesakeMathematics - Analysis of PDEs37K05Modelling and SimulationGradient catastrophe and elliptic umbilic catastrophe34M55FOS: MathematicsInitial value problemSettore MAT/07 - Fisica MatematicaEngineering(all)Mathematical PhysicsMathematicsG100Partial differential equationConjectureNonlinear Sciences - Exactly Solvable and Integrable SystemsHyperbolic and Elliptic systemsApplied MathematicsMathematical analysisQuasi-integrable systemsGeneral EngineeringMathematical Physics (math-ph)35Q55Nonlinear systemModeling and SimulationsymbolsExactly Solvable and Integrable Systems (nlin.SI)Hamiltonian (quantum mechanics)Gradient catastrophe and elliptic umbilic catastrophe; Hamiltonian PDEs; Hyperbolic and Elliptic systems; Painlevé equations; Quasi-integrable systemsAnalysis of PDEs (math.AP)
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The Principles of Canonical Mechanics

2010

Canonical mechanics is a central part of general mechanics, where one goes beyond the somewhat narrow framework of Newtonian mechanics with position coordinates in the three-dimensional space, towards a more general formulation of mechanical systems belonging to a much larger class. This is the first step of abstraction, leaving behind ballistics, satellite orbits, inclined planes, and pendulum-clocks; it leads to a new kind of description that turns out to be useful in areas of physics far beyond mechanics. Through d’Alembert’s principle we discover the concept of the Lagrangian function and the framework of Lagrangian mechanics that is built onto it. Lagrangian functions are particularly …

Hamiltonian mechanicsLegendre transformationsymbols.namesakePoisson bracketPhase spaceLagrangian mechanicssymbolsCanonical transformationMechanicsAnalytical dynamicsHamiltonian systemMathematics
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Bi-homogeneity and integrability of rational potentials

2020

Abstract In this paper we consider natural Hamiltonian systems with two degrees of freedom for which Hamiltonian function has the form H = 1 2 ( p 1 2 + p 2 2 ) + V ( q 1 , q 2 ) and potential V ( q 1 , q 2 ) is a rational function. Necessary conditions for the integrability of such systems are deduced from integrability of dominate term of the potential which usually is appropriately chosen homogeneous term of V. We show that introducing weights compatible with the canonical structure one can find new dominant terms which can give new necessary conditions for integrability. To deduce them we investigate integrability of a family of bi-homogeneous potentials which depend on two integer para…

Hamiltonian mechanicsPure mathematicsPolynomialDegree (graph theory)Integrable system010308 nuclear & particles physicsApplied MathematicsHomogeneous potentialsRational functionDifferential Galois theoryIntegrability01 natural sciencesHamiltonian systemsymbols.namesakeQuadratic equationIntegerSpecial functions0103 physical sciencessymbolsMSC 37J30[MATH]Mathematics [math]010306 general physicsAnalysisMathematicsJournal of Differential Equations
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Spatially localized solutions of the Hammerstein equation with sigmoid type of nonlinearity

2016

Abstract We study the existence of fixed points to a parameterized Hammerstein operator H β , β ∈ ( 0 , ∞ ] , with sigmoid type of nonlinearity. The parameter β ∞ indicates the steepness of the slope of a nonlinear smooth sigmoid function and the limit case β = ∞ corresponds to a discontinuous unit step function. We prove that spatially localized solutions to the fixed point problem for large β exist and can be approximated by the fixed points of H ∞ . These results are of a high importance in biological applications where one often approximates the smooth sigmoid by discontinuous unit step function. Moreover, in order to achieve even better approximation than a solution of the limit proble…

Heaviside step functionIterative methodApplied Mathematics010102 general mathematicsMathematical analysisSigmoid functionFixed point01 natural sciences010305 fluids & plasmasHamiltonian systemFunctional Analysis (math.FA)Mathematics - Functional AnalysisNonlinear systemsymbols.namesakeMathematics - Analysis of PDEs0103 physical sciencessymbolsFOS: MathematicsFitzHugh–Nagumo modelHomoclinic orbit0101 mathematicsAnalysisMathematicsAnalysis of PDEs (math.AP)
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Approximate renormalization-group transformation for Hamiltonian systems with three degrees of freedom

1999

We construct an approximate renormalization transformation that combines Kolmogorov-Arnold-Moser (KAM)and renormalization-group techniques, to analyze instabilities in Hamiltonian systems with three degrees of freedom. This scheme is implemented both for isoenergetically nondegenerate and for degenerate Hamiltonians. For the spiral mean frequency vector, we find numerically that the iterations of the transformation on nondegenerate Hamiltonians tend to degenerate ones on the critical surface. As a consequence, isoenergetically degenerate and nondegenerate Hamiltonians belong to the same universality class, and thus the corresponding critical invariant tori have the same type of scaling prop…

KAM TORI; RENORMALIZATION GROUP; STRANGE ATTRACTORSDegenerate energy levelsFOS: Physical sciencesKAM TORIRenormalization groupNonlinear Sciences - Chaotic DynamicsStrange nonchaotic attractorSTRANGE ATTRACTORSHamiltonian systemNonlinear Sciences::Chaotic DynamicsRenormalizationTransformation (function)RENORMALIZATION GROUPQuantum mechanicsChaotic Dynamics (nlin.CD)Invariant (mathematics)Settore MAT/07 - Fisica MatematicaMathematics::Symplectic GeometryScalingMathematicsMathematical physicsPhysical Review E
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