Search results for "Strange nonchaotic attractor"

showing 3 items of 3 documents

Hidden Strange Nonchaotic Attractors

2021

In this paper, it is found numerically that the previously found hidden chaotic attractors of the Rabinovich–Fabrikant system actually present the characteristics of strange nonchaotic attractors. For a range of the bifurcation parameter, the hidden attractor is manifestly fractal with aperiodic dynamics, and even the finite-time largest Lyapunov exponent, a measure of trajectory separation with nearby initial conditions, is negative. To verify these characteristics numerically, the finite-time Lyapunov exponents, ‘0-1’ test, power spectra density, and recurrence plot are used. Beside the considered hidden strange nonchaotic attractor, a self-excited chaotic attractor and a quasiperiodic at…

Mathematics::Dynamical SystemsGeneral MathematicsChaoticattraktoritLyapunov exponenthidden chaotic attractor01 natural sciencesStrange nonchaotic attractor010305 fluids & plasmassymbols.namesakeFractalRabinovich–Fabrikant system0103 physical sciencesAttractorComputer Science (miscellaneous)Statistical physicsdynaamiset systeemitRecurrence plot010301 acousticsEngineering (miscellaneous)BifurcationPhysicskaaosteorialcsh:Mathematicslcsh:QA1-939strange nonchaotic attractorself-excited attractorNonlinear Sciences::Chaotic DynamicsQuasiperiodic functionsymbolsfraktaalitMathematics
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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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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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