Search results for "Lyapunov exponent"

showing 10 items of 55 documents

Intermittent-Type Chaos in Nonsinusoidal Driven Oscillators

2000

The intermittent-type chaos occurring in rf- and dc- nonsinusoidal driven oscillators is investigated analytically and numerically. The attention is focused on a general class of oscillators in which the total potential VRP(,r) is the Remoissenet-Peyrard potential which has constant amplitude and is 2π-periodic in , and whose shape can be varied as a function of parameter r ( |r| < 1). A simple physical model for calculating analytically the Melnikov function is proposed. The onset of chaos is studied through an analysis of the phase space, a construction of the bifurcation diagram and a computation of the Lyapunov exponent. The parameter regions of chaotic behaviour predicted by the theore…

PhysicsComputationMathematical analysisChaoticFunction (mathematics)Lyapunov exponentCondensed Matter PhysicsBifurcation diagramAtomic and Molecular Physics and OpticsNonlinear Sciences::Chaotic Dynamicssymbols.namesakeAmplitudeClassical mechanicsPhase spacesymbolsConstant (mathematics)Mathematical PhysicsPhysica Scripta
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Chaotic Cyclotron and Hall Trajectories Due to Spin-Orbit Coupling

2020

We demonstrate that the synergistic effect of a gauge field, Rashba spin-orbit coupling (SOC), and Zeeman splitting can generate chaotic cyclotron and Hall trajectories of particles. The physical origin of the chaotic behavior is that the SOC produces a spin-dependent (so-called anomalous) contribution to the particle velocity and the presence of Zeeman field reduces the number of integrals of motion. By using analytical and numerical arguments, we study the conditions of chaos emergence and report the dynamics both in the regular and chaotic regimes. {We observe the critical dependence of the dynamic patterns (such as the chaotic regime onset) on small variations in the initial conditions …

PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsHall eectCyclotronChaoticGeneral Physics and AstronomyFOS: Physical sciencesLyapunov exponentSpin–orbit interactionchaotic trajectoriesNonlinear Sciences - Chaotic Dynamicslaw.inventionspin-orbit couplingNonlinear Sciences::Chaotic Dynamicssymbols.namesakelawHall effectanomalous velocitiesQuantum electrodynamicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)Lyapunov expo-nentssymbolsChaotic Dynamics (nlin.CD)Annalen der Physik
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Linear inverse filtering improves spatial separation of nonlinear brain dynamics: a simulation study.

2000

We examined topographic variations in nonlinear measures based on scalp voltages, which were generated by two simulated current dipoles each placed in a different hemisphere of a spherical volume conductor (three-shell model). Dipole dynamics were that of a three-torus and the x-component of the Lorenz-system and scalp voltage were calculated for a configuration of 29 electrode positions. Although estimates for correlation dimension D2 and Lyapunov exponent L1 were close to the theoretical values for the original time series, the simulated scalp voltage data showed almost no topographic resolution of dipole positions. In order to enhance topographic differentiation, we constructed linear in…

PhysicsCorrelation dimensionBrain MappingQuantitative Biology::Neurons and CognitionSeries (mathematics)General NeurosciencePhysics::Medical PhysicsMathematical analysisModels NeurologicalInverseBrainElectroencephalographyLyapunov exponentNonlinear systemsymbols.namesakeDipoleNonlinear DynamicsStatisticssymbolsHumansComputer SimulationFocus (optics)Image resolutionJournal of neuroscience methods
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Rich dynamics and anticontrol of extinction in a prey-predator system

2019

This paper reveals some new and rich dynamics of a two-dimensional prey-predator system and to anticontrol the extinction of one of the species. For a particular value of the bifurcation parameter, one of the system variable dynamics is going to extinct, while another remains chaotic. To prevent the extinction, a simple anticontrol algorithm is applied so that the system orbits can escape from the vanishing trap. As the bifurcation parameter increases, the system presents quasiperiodic, stable, chaotic and also hyperchaotic orbits. Some of the chaotic attractors are Kaplan-Yorke type, in the sense that the sum of its Lyapunov exponents is positive. Also, atypically for undriven discrete sys…

PhysicsExtinctionPhase portraitApplied MathematicsMechanical EngineeringChaoticFOS: Physical sciencesAerospace EngineeringOcean EngineeringLyapunov exponentNonlinear Sciences - Chaotic Dynamics01 natural sciencesStrange nonchaotic attractorNonlinear Sciences::Chaotic Dynamicssymbols.namesakeControl and Systems EngineeringQuasiperiodic function0103 physical sciencesAttractorsymbolsStatistical physicsChaotic Dynamics (nlin.CD)Electrical and Electronic Engineering010301 acousticsBifurcation
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Chaotic Antiferromagnetic Nano-Oscillator driven by Spin-Torque

2021

We theoretically describe the behavior of a terahertz nano-oscillator based on an anisotropic antiferromagnetic dynamical element driven by spin torque. We consider the situation when the polarization of the spin-current is perpendicular to the external magnetic field applied along the anisotropy easy-axis. We determine the domain of the parametric space (field, current) where the oscillator demonstrates chaotic dynamics. Characteristics of the chaotic regimes are analyzed using conventional techniques such as spectra of the Lyapunov exponents. We show that the threshold current of the chaos appearance is particularly low in the vicinity of the spin-flop transition. In this regime, we consi…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsField (physics)ChaoticFOS: Physical sciences02 engineering and technologyLyapunov exponent021001 nanoscience & nanotechnologyNonlinear Sciences - Chaotic Dynamics01 natural sciencesMagnetic fieldNonlinear Sciences::Chaotic Dynamicssymbols.namesakeMagnetic anisotropyCondensed Matter - Strongly Correlated ElectronsQuasiperiodic functionPhase space0103 physical sciencessymbolsChaotic Dynamics (nlin.CD)010306 general physics0210 nano-technologySpin-½
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A criterion for zero averages and full support of ergodic measures

2018

International audience; Consider a homeomorphism $f$ defined on a compact metric space $X$ and a continuous map $\phi\colon X \to \mathbb{R}$. We provide an abstract criterion, called control at any scale with a long sparse tail for a point $x\in X$ and the map $\phi$, which guarantees that any weak* limit measure $\mu$ of the Birkhoff average of Dirac measures $\frac1n\sum_0^{n-1}\delta(f^i(x))$ s such that $\mu$-almost every point $y$ has a dense orbit in $X$ and the Birkhoff average of $\phi$ along the orbit of $y$ is zero.As an illustration of the strength of this criterion, we prove that the diffeomorphisms with nonhyperbolic ergodic measures form a $C^1$-open and dense subset of the s…

Pure mathematics37D25 37D30 37D35 28D99Mathematics::Dynamical SystemsDense setGeneral MathematicsNonhyperbolic measure[ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]MSC: 37D25 37D35 37D30 28D99[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Partial hyperbolicity01 natural sciencesMeasure (mathematics)FOS: MathematicsErgodic theoryHomoclinic orbit0101 mathematicsMathematics - Dynamical SystemsMathematicsTransitivity010102 general mathematicsZero (complex analysis)Ergodic measure010101 applied mathematicsCompact spaceHomeomorphism (graph theory)Birkhoff averageOrbit (control theory)Lyapunov exponent
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Integrability via Reversibility

2017

Abstract A class of left-invariant second order reversible systems with functional parameter is introduced which exhibits the phenomenon of robust integrability: an open and dense subset of the phase space is filled with invariant tori carrying quasi-periodic motions, and this behavior persists under perturbations within the class. Real-analytic volume preserving systems are found in this class which have positive Lyapunov exponents on an open subset, and the complement filled with invariant tori.

Pure mathematicsClass (set theory)Dense setGeneral Physics and AstronomyLyapunov exponentDynamical Systems (math.DS)IntegrabilityCoexistence of integrability and chaotic behavior01 natural sciencessymbols.namesakeReversibility0103 physical sciencesFOS: MathematicsOrder (group theory)0101 mathematicsInvariant (mathematics)Mathematics - Dynamical SystemsMathematical PhysicsMathematicsComplement (set theory)010102 general mathematicsTorusPhase spacesymbols010307 mathematical physicsGeometry and Topology
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Periodic measures and partially hyperbolic homoclinic classes

2019

In this paper, we give a precise meaning to the following fact, and we prove it: $C^1$-open and densely, all the non-hyperbolic ergodic measures generated by a robust cycle are approximated by periodic measures. We apply our technique to the global setting of partially hyperbolic diffeomorphisms with one dimensional center. When both strong stable and unstable foliations are minimal, we get that the closure of the set of ergodic measures is the union of two convex sets corresponding to the two possible $s$-indices; these two convex sets intersect along the closure of the set of non-hyperbolic ergodic measures. That is the case for robustly transitive perturbation of the time one map of a tr…

Pure mathematicsMathematics::Dynamical SystemsGeneral MathematicsClosure (topology)Dynamical Systems (math.DS)01 natural sciencespartial hyperbolicityquasi-hyperbolic stringBlenderFOS: Mathematicsnon-hyperbolic measureErgodic theoryHomoclinic orbitMathematics - Dynamical Systems0101 mathematics[MATH]Mathematics [math]ergodic measureperiodic measureMathematicsfoliationsTransitive relationApplied MathematicsMSC (2010): Primary 37D30 37C40 37C50 37A25 37D25010102 general mathematicsRegular polygonTorusstabilityFlow (mathematics)systemsDiffeomorphismrobust cycleLyapunov exponent
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Chaotic Properties of Dilute Two and Three Dimensional Random Lorentz Gases II: Open Systems

2000

We calculate the spectrum of Lyapunov exponents for a point particle moving in a random array of fixed hard disk or hard sphere scatterers, i.e. the disordered Lorentz gas, in a generic nonequilibrium situation. In a large system which is finite in at least some directions, and with absorbing boundary conditions, the moving particle escapes the system with probability one. However, there is a set of zero Lebesgue measure of initial phase points for the moving particle, such that escape never occurs. Typically, this set of points forms a fractal repeller, and the Lyapunov spectrum is calculated here for trajectories on this repeller. For this calculation, we need the solution of the recently…

Random arrayLorentz transformationMathematical analysisChaoticFOS: Physical sciencesLyapunov exponentNonlinear Sciences - Chaotic DynamicsCollision operatorEntropy (classical thermodynamics)symbols.namesakesymbolsChaotic Dynamics (nlin.CD)Lyapunov spectrumMathematics
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Visualization of Parameter Sensitivity of 2D Time-Dependent Flow

2018

In this paper, we present an approach to analyze 1D parameter spaces of time-dependent flow simulation ensembles. By extending the concept of the finite-time Lyapunov exponent to the ensemble domain, i.e., to the parameter that gives rise to the ensemble, we obtain a tool for quantitative analysis of parameter sensitivity both in space and time. We exemplify our approach using 2D synthetic examples and computational fluid dynamics ensembles.

SpacetimeComputer sciencebusiness.industry020207 software engineering02 engineering and technologyLyapunov exponentComputational fluid dynamicsDomain (mathematical analysis)Visualizationsymbols.namesakeFlow (mathematics)0202 electrical engineering electronic engineering information engineeringsymbolsTime dependent flowStatistical physicsSensitivity (control systems)business
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