0000000000123840

AUTHOR

M. Govin

showing 5 related works from this author

Kolmogorov-Arnold-Moser–Renormalization-Group Analysis of Stability in Hamiltonian Flows

1997

We study the stability and breakup of invariant tori in Hamiltonian flows using a combination of Kolmogorov-Arnold-Moser (KAM) theory and renormalization-group techniques. We implement the scheme numerically for a family of Hamiltonians quadratic in the actions to analyze the strong coupling regime. We show that the KAM iteration converges up to the critical coupling at which the torus breaks up. Adding a renormalization consisting of a rescaling of phase space and a shift of resonances allows us to determine the critical coupling with higher accuracy. We determine a nontrivial fixed point and its universality properties.

PhysicsKolmogorov–Arnold–Moser theoremFOS: Physical sciencesGeneral Physics and AstronomyTorusRenormalization groupFixed pointNonlinear Sciences - Chaotic DynamicsUniversality (dynamical systems)Renormalizationsymbols.namesakeQuantum mechanicsPhase spacesymbolsChaotic Dynamics (nlin.CD)Hamiltonian (quantum mechanics)Mathematics::Symplectic GeometryMathematical physicsPhysical Review Letters
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Convergence of iterative methods in perturbation theory

1995

We discuss iterative KAM type methods for eigenvalue problems in finite dimensions. We compare their convergence properties with those of straight forward power series expansions.

Inverse iterationPower seriesSingular perturbationsymbols.namesakeIterative methodPreconditionerConvergence (routing)Mathematical analysissymbolsPerturbation theoryPoincaré–Lindstedt methodMathematics
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Domains of Convergence of Kam Type Iterations for Eigenvalue Problems

1999

The KAM technique was first introduced to deal with small denominator problems appearing in perturbation of invariant tori in classical mechanics [1, 2]. Similar methods were later applied to many different problems, like e.g. eigenvalue problems for time dependent problems in the Floquet representation [3, 4, 5, 6]. Most of the known results are valid for sufficiently small perturbation of some simple (integrable) system. The phenomena arising for large perturbations, in particular critical perturbations at which a given torus loses its stability, have been discussed in the framework of some approximate schemes inspired in renormalization group ideas [7, 8, 9]. In this framework, an iterat…

Floquet theoryDiscrete mathematicsIntegrable systemPerturbation (astronomy)Applied mathematicsTorusUnitary transformationRenormalization groupFixed pointEigenvalues and eigenvectorsMathematics
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Universality for the breakup of invariant tori in Hamiltonian flows

1998

In this article, we describe a new renormalization-group scheme for analyzing the breakup of invariant tori for Hamiltonian systems with two degrees of freedom. The transformation, which acts on Hamiltonians that are quadratic in the action variables, combines a rescaling of phase space and a partial elimination of irrelevant (non-resonant) frequencies. It is implemented numerically for the case applying to golden invariant tori. We find a nontrivial fixed point and compute the corresponding scaling and critical indices. If one compares flows to maps in the canonical way, our results are consistent with existing data on the breakup of golden invariant circles for area-preserving maps.

Mathematical analysisFOS: Physical sciencesFixed pointNonlinear Sciences - Chaotic DynamicsBreakup01 natural sciences010305 fluids & plasmasUniversality (dynamical systems)Hamiltonian systemsymbols.namesakeQuadratic equationPhase space0103 physical sciencessymbolsChaotic Dynamics (nlin.CD)010306 general physicsHamiltonian (quantum mechanics)ScalingMathematical physicsMathematicsPhysical Review E
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Convergence of KAM iterations for counterterm problems

1998

Abstract We analyse two iterative KAM methods for counterterm problems for finite-dimensional matrices. The starting point for these methods is the KAM iteration for Hamiltonians linear in the action variable in classical mechanics. We compare their convergence properties when a perturbation parameter is varied. The first method has no fixed points beyond a critical value of the perturbation parameter. The second one has fixed points for arbitrarily large perturbations. We observe different domains of attraction separated by Julia sets.

Arbitrarily largeGeneral MathematicsApplied MathematicsMathematical analysisGeneral Physics and AstronomyPerturbation (astronomy)Statistical and Nonlinear PhysicsFixed pointAction variableCritical valueJulia setMathematicsChaos, Solitons & Fractals
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