Search results for " 37D30"

showing 10 items of 14 documents

Partially hyperbolic diffeomorphisms with a uniformly compact center foliation: the quotient dynamics

2016

We show that a partially hyperbolic$C^{1}$-diffeomorphism$f:M\rightarrow M$with a uniformly compact$f$-invariant center foliation${\mathcal{F}}^{c}$is dynamically coherent. Further, the induced homeomorphism$F:M/{\mathcal{F}}^{c}\rightarrow M/{\mathcal{F}}^{c}$on the quotient space of the center foliation has the shadowing property, i.e. for every${\it\epsilon}>0$there exists${\it\delta}>0$such that every${\it\delta}$-pseudo-orbit of center leaves is${\it\epsilon}$-shadowed by an orbit of center leaves. Although the shadowing orbit is not necessarily unique, we prove the density of periodic center leaves inside the chain recurrent set of the quotient dynamics. Other interesting proper…

010101 applied mathematicsPure mathematicsMSC: 37D30 37C15Applied MathematicsGeneral Mathematics010102 general mathematics[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]0101 mathematics01 natural sciencesQuotientMathematics
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A mechanism for ejecting a horseshoe from a partially hyperbolic chain recurrence class

2022

We give a $C^1$-perturbation technique for ejecting an a priori given finite set of periodic points preserving a given finite set of homo/hetero-clinic intersections from a chain recurrence class of a periodic point. The technique is first stated under a simpler setting called Markov iterated function system, a two dimensional iterated function system in which the compositions are chosen in Markovian way. Then we apply the result to the setting of three dimensional partially hyperbolic diffeomorphisms.

37B25 37D30 37G35FOS: Mathematics[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Mathematics - Dynamical Systems
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Aperiodic chain recurrence classes of $C^1$-generic diffeomorphisms

2022

We consider the space of $C^1$-diffeomorphims equipped with the $C^1$-topology on a three dimensional closed manifold. It is known that there are open sets in which $C^1$-generic diffeomorphisms display uncountably many chain recurrences classes, while only countably many of them may contain periodic orbits. The classes without periodic orbits, called aperiodic classes, are the main subject of this paper. The aim of the paper is to show that aperiodic classes of $C^1$-generic diffeomorphisms can exhibit a variety of topological properties. More specifically, there are $C^1$-generic diffeomorphisms with (1) minimal expansive aperiodic classes, (2) minimal but non-uniquely ergodic aperiodic c…

FOS: Mathematics[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Mathematics - Dynamical Systems37C20 37D30 57M30
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Internal perturbations of homoclinic classes:non-domination, cycles, and self-replication

2010

Conditions are provided under which lack of domination of a homoclinic class yields robust heterodimensional cycles. Moreover, so-called viral homoclinic classes are studied. Viral classes have the property of generating copies of themselves producing wild dynamics (systems with infinitely many homoclinic classes with some persistence). Such wild dynamics also exhibits uncountably many aperiodic chain recurrence classes. A scenario (related with non-dominated dynamics) is presented where viral homoclinic classes occur. A key ingredient are adapted perturbations of a diffeomorphism along a periodic orbit. Such perturbations preserve certain homoclinic relations and prescribed dynamical prope…

Nonlinear Sciences::Chaotic DynamicsMathematics::Dynamical Systems37C29 37D20 37D30[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]FOS: Mathematics[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)Mathematics - Dynamical Systems
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Flexible periodic points

2014

We define the notion of ${\it\varepsilon}$-flexible periodic point: it is a periodic point with stable index equal to two whose dynamics restricted to the stable direction admits ${\it\varepsilon}$-perturbations both to a homothety and a saddle having an eigenvalue equal to one. We show that an ${\it\varepsilon}$-perturbation to an ${\it\varepsilon}$-flexible point allows us to change it to a stable index one periodic point whose (one-dimensional) stable manifold is an arbitrarily chosen $C^{1}$-curve. We also show that the existence of flexible points is a general phenomenon among systems with a robustly non-hyperbolic two-dimensional center-stable bundle.

Pure mathematics37C29 37D30Applied MathematicsGeneral MathematicsBundlePhenomenonFOS: MathematicsDynamical Systems (math.DS)Mathematics - Dynamical SystemsMathematicsErgodic Theory and Dynamical Systems
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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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Anomalous partially hyperbolic diffeomorphisms III: Abundance and incoherence

2020

Let $M$ be a closed 3-manifold which admits an Anosov flow. In this paper we develop a technique for constructing partially hyperbolic representatives in many mapping classes of $M$. We apply this technique both in the setting of geodesic flows on closed hyperbolic surfaces and for Anosov flows which admit transverse tori. We emphasize the similarity of both constructions through the concept of $h$-transversality, a tool which allows us to compose different mapping classes while retaining partial hyperbolicity. In the case of the geodesic flow of a closed hyperbolic surface $S$ we build stably ergodic, partially hyperbolic diffeomorphisms whose mapping classes form a subgroup of the mapping…

Pure mathematics37D30Similarity (geometry)Mathematics::Dynamical SystemsGeodesic[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)dynamical coherenceMSC Primary: 37C15 37D3037C1501 natural sciencessymbols.namesake0103 physical sciencesFOS: MathematicsErgodic theoryMathematics - Dynamical Systems[MATH]Mathematics [math]0101 mathematicsComputingMilieux_MISCELLANEOUSMathematicsConjecture010102 general mathematicsSurface (topology)Mathematics::Geometric Topologystable ergodicityMapping class groupFlow (mathematics)Poincaré conjecturesymbols010307 mathematical physicsGeometry and Topologypartially hyperbolic diffeomorphisms
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Anomalous partially hyperbolic diffeomorphisms I: dynamically coherent examples

2016

We build an example of a non-transitive, dynamically coherent partially hyperbolic diffeomorphism $f$ on a closed $3$-manifold with exponential growth in its fundamental group such that $f^n$ is not isotopic to the identity for all $n\neq 0$. This example contradicts a conjecture in \cite{HHU}. The main idea is to consider a well-understood time-$t$ map of a non-transitive Anosov flow and then carefully compose with a Dehn twist.

Pure mathematicsFundamental groupMathematics::Dynamical SystemsGeneral Mathematics[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]MSc: 37D30[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Dynamical Systems (math.DS)01 natural sciencesIdentity (music)Exponential growth0103 physical sciencesFOS: MathematicsMathematics - Dynamical Systems0101 mathematicsMathematicsConjecture010102 general mathematicsClassificationMathematics::Geometric TopologyDehn twistFlow (mathematics)Partially hyperbolic diffeomorphisms010307 mathematical physicsDiffeomorphism
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Stabilization of heterodimensional cycles

2011

We consider diffeomorphisms $f$ with heteroclinic cycles associated to saddles $P$ and $Q$ of different indices. We say that a cycle of this type can be stabilized if there are diffeomorphisms close to $f$ with a robust cycle associated to hyperbolic sets containing the continuations of $P$ and $Q$. We focus on the case where the indices of these two saddles differ by one. We prove that, excluding one particular case (so-called twisted cycles that additionally satisfy some geometrical restrictions), all such cycles can be stabilized.

Pure mathematicsMathematics::Dynamical Systems37C29 37D20 37D30Applied MathematicsFOS: MathematicsGeneral Physics and AstronomyStatistical and Nonlinear PhysicsDynamical Systems (math.DS)Mathematics - Dynamical SystemsType (model theory)Focus (optics)Mathematical PhysicsMathematicsNonlinearity
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On the existence of attractors

2009

On every compact 3-manifold, we build a non-empty open set $\cU$ of $\Diff^1(M)$ such that, for every $r\geq 1$, every $C^r$-generic diffeomorphism $f\in\cU\cap \Diff^r(M)$ has no topological attractors. On higher dimensional manifolds, one may require that $f$ has neither topological attractors nor topological repellers. Our examples have finitely many quasi attractors. For flows, we may require that these quasi attractors contain singular points. Finally we discuss alternative definitions of attractors which may be better adapted to generic dynamics.

Pure mathematicsMathematics::Dynamical SystemsApplied MathematicsGeneral MathematicsMathematical analysisOpen setDynamical Systems (math.DS)Nonlinear Sciences::Chaotic Dynamics37C05 37C20 37C25 37C29 37D30AttractorFOS: MathematicsDiffeomorphismMathematics - Dynamical SystemsMathematics::Symplectic GeometryMathematics
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