Search results for "Stable manifold"

showing 9 items of 9 documents

Persistence of Asteroids After a Close Encounter

1999

We present here a first approximation to the planar circular restricted 2 + 2 problem. In this four body problem, we consider that the two secondaries do not affect the primaries but they do influence each other. It can be seen as a model for near collision orbits of two asteroids if the primaries are the Sun and Jupiter ([3], [5]). In particular, we analyze the values of the Jacobi constant of the two asteroids before and after the close approach.

JupiterPhysicsAsteroidPhysics::Space PhysicsInvariant manifoldAstrophysics::Earth and Planetary AstrophysicsAstrophysicsClose encounterPersistence (discontinuity)Constant (mathematics)CollisionStable manifold
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Critical Attractor and Universality in a Renormalization Scheme for Three Frequency Hamiltonian Systems

1998

We study an approximate renormalization-group transformation to analyze the breakup of invariant tori for three degrees of freedom Hamiltonian systems. The scheme is implemented for the spiral mean torus. We find numerically that the critical surface is the stable manifold of a critical nonperiodic attractor. We compute scaling exponents associated with this fixed set, and find that they can be expected to be universal.

PhysicsCritical phenomenaGeneral Physics and AstronomyFOS: Physical sciencesTorusNonlinear Sciences - Chaotic DynamicsStable manifoldUniversality (dynamical systems)Hamiltonian systemRenormalizationAttractorChaotic Dynamics (nlin.CD)Critical exponentMathematics::Symplectic GeometryMathematical physics
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Structural similarities and differences among attractors and their intensity maps in the laser-Lorenz model

1995

Abstract Numerical studies of the laser-Lorenz model using parameters reasonably accessible for recent experiments with a single mode homogeneously broadened laser demonstrate that the form of the return map of successive peak values of the intensity changes from a sharply cusped map in resonance to a map with a smoothly rounded maximum as the laser is detuned into the period doubling regime. This transformation appears to be related to the disappearance (with detuning) of the heteroclinic structural basis for the stable manifold which exists in resonance. This is in contrast to the evidence reported by Tang and Weiss (Phys. Rev. A 49 (1994) 1296) of a cusped map for both the period doublin…

PhysicsPeriod-doubling bifurcationbusiness.industrySingle-mode optical fiberLaserResonance (particle physics)Atomic and Molecular Physics and OpticsStable manifoldElectronic Optical and Magnetic Materialslaw.inventionIntensity (physics)Nonlinear Sciences::Chaotic DynamicsTransformation (function)OpticslawAttractorPhysics::Atomic PhysicsElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessOptics Communications
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Robust control of unstable nonlinear quantum systems

2020

Adiabatic passage is a standard tool for achieving robust transfer in quantum systems. We show that, in the context of driven nonlinear Hamiltonian systems, adiabatic passage becomes highly non-robust when the target is unstable. We show this result for a generic (1:2) resonance, for which the complete transfer corresponds to a hyperbolic fixed point in the classical phase space featuring an adiabatic connectivity strongly sensitive to small perturbations of the model. By inverse engineering, we devise high-fidelity and robust partially non-adiabatic trajectories. They localize at the approach of the target near the stable manifold of the separatrix, which drives the dynamics towards the ta…

PhysicsQuantum PhysicsNonlinear opticsFOS: Physical sciences01 natural sciencesResonance (particle physics)Stable manifold010305 fluids & plasmasNonlinear system0103 physical sciencesStatistical physicsRobust control010306 general physicsAdiabatic processQuantum Physics (quant-ph)QuantumHyperbolic equilibrium pointPhysical Review A
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On the saddle loop bifurcation

1990

It is shown that the set of C∞ (generic) saddle loop bifurcations has a unique modulus of stability γ ≥]0, 1[∪]1, ∞[ for (C0, Cr)-equivalence, with 1≤r≤∞. We mean for an equivalence (x,μ) ↦ (h(x,μ), ϕ(μ)) with h continuous and ϕ of class Cr. The modulus γ is the ratio of hyperbolicity at the saddle point of the connection. Already asking ϕ to be a lipeomorphism forces two saddle loop bifurcations to have the same modulus, while two such bifurcations with the same modulus are (C0,±Identity)-equivalent.

PhysicsSaddle pointMathematical analysisModulusVector fieldBifurcation diagramEngineering physicsBifurcationStable manifoldSaddle
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Non-immersion theorem for a class of hyperbolic manifolds

1998

Abstract It is proved that a non-simply-connected complete hyperbolic manifold cannot be isometrically immersed in a Euclidean space with a flat normal connection. In particular, the complete hyperbolic manifold M n with π 1 ( M ) ≠ 0 cannot be isometrically immersed in R 2 n − 1 .

Pure mathematicsHyperbolic groupHyperbolic spaceMathematical analysisHyperbolic 3-manifoldHyperbolic manifoldUltraparallel theoremMathematics::Geometric TopologyRelatively hyperbolic groupStable manifoldComputational Theory and MathematicsMathematics::Metric GeometryMathematics::Differential GeometryGeometry and TopologyAnalysisHyperbolic equilibrium pointMathematicsDifferential Geometry and its Applications
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Renormalization-group analysis for the transition to chaos in Hamiltonian systems

2002

Abstract We study the stability of Hamiltonian systems in classical mechanics with two degrees of freedom by renormalization-group methods. One of the key mechanisms of the transition to chaos is the break-up of invariant tori, which plays an essential role in the large scale and long-term behavior. The aim is to determine the threshold of break-up of invariant tori and its mechanism. The idea is to construct a renormalization transformation as a canonical change of coordinates, which deals with the dominant resonances leading to qualitative changes in the dynamics. Numerical results show that this transformation is an efficient tool for the determination of the threshold of the break-up of…

RenormalizationPhysicsFractalQuantum mechanicsGeneral Physics and AstronomyTorusInvariant (physics)Renormalization groupMathematics::Symplectic GeometryStable manifoldHamiltonian systemUniversality (dynamical systems)Mathematical physicsPhysics Reports
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Existence of a traveling wave solution in a free interface problem with fractional order kinetics

2021

Abstract In this paper we consider a system of two reaction-diffusion equations that models diffusional-thermal combustion with stepwise ignition-temperature kinetics and fractional reaction order 0 α 1 . We turn the free interface problem into a scalar free boundary problem coupled with an integral equation. The main intermediary step is to reduce the scalar problem to the study of a non-Lipschitz vector field in dimension 2. The latter is treated by qualitative topological methods based on the Poincare-Bendixson Theorem. The phase portrait is determined and the existence of a stable manifold at the origin is proved. A significant result is that the settling time to reach the origin is fin…

Settling timeScalar (mathematics)01 natural sciencesPoincare-Bendixson TheoremTraveling wave solutionsMathematics - Analysis of PDEsDimension (vector space)Free boundary problemFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Trapping triangles0101 mathematicsMathematicsPhase portraitApplied Mathematics010102 general mathematicsMathematical analysisIntegral equationStable manifoldDiffusional-thermal combustionFree interface problems010101 applied mathematicsVector fieldFractional order kineticsAnalysisAnalysis of PDEs (math.AP)
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Collision Orbits in the Isosceles Rectilinear Restricted Problem

1995

In the study of the Collinear Three-Body Problem, McGehee (1974) introduced a new set of coordinates which had the effect of blowing up the triple collision singularity. Subsequently, his method has been used to analyze some other collision or singularities. Recently, Wang (1986) introduced another transformation which differs from the McGehee’s coordinates in the fact that the blowing-up factor is now the potential function, U, instead of the moment of inertia, I. Meyer and Wang (1993) have applied this method to the Restricted Isosceles Three-body Problem with positive energy and Cors and Llibre (1994) to the hyperbolic restricted three-body problem. In this paper we study the singulariti…

SingularityClassical mechanicsBounded functionMathematical analysisIsosceles triangleGravitational singularityNegative energyFunction (mathematics)Stable manifoldMathematicsBlowing up
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