Entropy of C 1 -diffeomorphisms without dominated splitting
|
|
- Josephine Morrison
- 5 years ago
- Views:
Transcription
1 Entropy of C 1 -diffeomorphisms without dominated splitting Jérôme Buzzi (CNRS & Université Paris-Sud) joint with S. CROVISIER and T. FISHER June 15, 2017 Beyond Uniform Hyperbolicity - Provo, UT
2 Outline Introduction Understanding topological entropy Topological and measured entropies Creating a horseshoe Localized perturbative theorem Ingredients of the proof Dissipative diffeomorphisms Horseshoe entropy Infinitely many homoclinic classes Conservative diffeomorphisms Entropy formulas Instability, continuity,... Borel classification Conclusion
3 Understanding topological entropy f : M M compact, connected, without boundary Topological Entropy (Adler-McAndrew-Konheim 1968) h top : Diff r (M) [0, ) How does it vary? - continuity: Misiurewicz,Katok (low d); Newhouse,Yomdin C - local constancy: stability beyond hyperbolicity (B-Fisher) - robust instability (diffeos not approximated by local constancy)? What are its sources? - homology: Shub s Entropy conjecture - volume growth: Yomdin, Newhouse C - combinatorics through Markov partitions: Bowen - combinatorics through horseshoes: Katok Diff 1+α (M 2 ) How does it classify? - Generators: Jewett-Krieger, Hochman, Burguet-Downarowicz - Almost... conjugacy: Adler-Marcus, Boyle-B-Gomez Which values does it takes?
4 Topological and measure entropies - Definitions f : M M C 0, compact, µ P erg (f ) Topological Entropy (Adler-McAndrew-Konheim 1965; Bowen 1971) h top (f ) = lim ɛ 0+ h top (f, ɛ) h top (f, ɛ) = lim sup n 1 n log r f (ɛ, n, M) Measured Entropy (Kolmogorov-Sinai 1958; Katok 1980) h(f, µ) = lim ɛ 0+ h(f, µ, ɛ) h(f, µ, ɛ) = lim sup n 1 n log r f (ɛ, n, µ) Tail Entropy (Misiurewicz-Bowen 1973) h (f ) = lim ɛ 0+ h (f, ɛ) h 1 (f, ɛ) = sup h top(f, B f (x, ɛ, )) = lim lim sup x M δ 0 n Variational principle (Goodman 1971) h top (f ) = sup{h(f, µ) : µ P erg (f )} Measure maximizing the entropy (mme) n sup x M r f (δ, n, B f (x, ɛ, n)) µ max P erg (f ) with h(f, µ max ) = sup{h(f, µ) : µ P erg (f )} Newhouse: C = existence
5 Main Theorem For µ P erg (f ), f Diff 1 (M), M closed Lyapunov Exponents λ 1 (f, µ) λ 2 (f, µ) λ d (f, µ) Ruelle s inequality: h(f, µ) (f, µ) := min ( i λ i(f, µ) +, i λ i(f, µ) ) Main Theorem (B-Crovisier-Fisher) U a neighborhood of f in Diff 1 (M), Diff 1 vol(m) or Diff 1 ω(m) O periodic orbit with large period and no strong dominated splitting Then, for each U O, there is a horseshoe O K U for g U s.t. h top (g, K) (g, O) = (f, O) Moreover: {g f } U \ O; can preserve a homoclinic relation Remark Optimal : lim sup g f h top (g) sup µ (f, µ) Remark Specific to C 1 -topology: tools; factor 1/r in C r Locally uniform bounds on required period, domination - Newhouse 1978 (d = 2); - Catalan-Tahzibi 2014 (symplectic, entropy min i ( λ i (f, O) )) (see also: Catalan 2016)
6 Tools for localized perturbations - Perturbations of periodic linear cocycles (Bochi-Bonatti, Gourmelon, new for symplectic) - making spectrum simple with rational angles; - mixing the stable (unstable) exponents - creating a small angle - Local support with homoclinic connection, form or symplectic form (Gourmelon): - Franks Lemma with linearization (Avila for volume-preserving) - Homoclinic tangency from lack of domination (Gourmelon) Localized perturbations of conservative C 1 diffeomorphisms, arxiv:1612:06914
7 Proof - Part I: circular permutation f Diff 1 (M) with O(p) a long periodic orbit with weak domination Use previous tools to create, by perturbations: 1. Transverse homoclinic point and locally linear horseshoe K 0 p 2. Point x K 0 with large period and Df π(x) x = Λ s Id E s Λ u Id E u 3. Homoclinic tangency z for O(x) 4. Linearize around O(x) so loc. invariant E 1... E }{{ k } E s 5. With F = T z W s (x) T z W u (x) assumed to be 1-d: T z W s (x) = F F s 1 F s k 1 T z W u (x) = F u 1 F u k d 1 F T z M = F (F s 1 F s k 1 ) G (F u 1 F u k d 1 ) E k+1... E d }{{} E u 6. Using Df π(x) =homothety homothety and F F u 1 F u k d 1 E s : Perturb future of z to get F E 1, Fi s E i+1 and G E k+1, Fj u E k+1+j Similarly in the past Fi s E i, G E k, Fj u E k+j, F E d Conclusion τ Wloc u (x) f m Wloc s (x) s.t. Df m τ.e i = E i+1 (E d+1 = E 1 )
8 Proof - Part II: entropy from exponents Case d = 3, k = 2 (λ 1 < λ 2 < 0 < λ 3 ) g n+m e3 g l+n e1 e2 δ 1 = δ, δ 2 = e nλ1, δ 3 = δe λ3 n Image by f n has height along e 1 : δe (λ1+λ2)n Wiggles (x 1,..., x d ) (x 1,..., x k, x k+1 + H cos(πnx 1 ), x k+2,..., x d ) - to cross: H C(e (λ1+λ2)n + e λ3n )δ - to be C 1 -small: N = o(h 1 ) Entropy log N n max( λ 1 λ 2, λ 3 ) = (f, O(x))
9 Application 1: C 1 horseshoes from LACK of domination Let f Diff 1 (M) be generic (ie, belonging to dense G δ in Diff 1 (M)) Theorem (B-Crovisier-Fisher) For any µ P erg (f ), if suppµ has no dominated splitting, then are horseshoes K n approximating µ: (i) in entropy; (ii) in Hausdorff distance; (iii) in weak-star topology Compare Katok C 1+ ; Gan, Gelfert C 1 + adapted dominated splitting Remark Does not say that K n supp(µ) or homoclinically related Ingredients of the proof: - Ergodic closing lemma with control of exponents - Main theorem
10 Application 2: Infinitely many homoclinic classes Homoclinic relation and classes for hyperbolic periodic orbit O: O O W s (O) W u (O ) et W u (O) W s (O ) HC(O) := O O O compact, invariant, transitive Theorem (B-Crovisier-Fisher) f Diff 1 (M) generic Any HC(O) without dominated splitting is accumulated by infinitely many homoclinic classes with entropy bounded away from zero More precisely, lim inf n h top (HC(O n )) sup O O (f, O ) Remark Newhouse s theorem would suffice (smaller bound) Ingredients: - O O with (O ) > (O), long period, weak domination - Franks Lemma and linear perturbation to make O a sink/source - undo the perturbation inside the basin - Main Theorem
11 Application 3: Entropy formulas in conservative settings M closed manifold with dim d 2, ω volume or symplectic form Let E 1 ω(m) := int({f Diff 1 ω(m) : no domination}) Theorem (B-Crovisier-Fisher) The topological entropy of a generic f E 1 ω(m) is equal to: (1) sup{h top (f, K) : K horseshoe} (2) sup{ (f, O) : O periodic orbit} (3) max 0<k<d lim n 1 n log sup E G k (TM) Jac(f n, E) generalizes, strengthens Catalan-Tahzibi (2014) Ingredients of the proof - sup K h top (K) h top (f ) = sup µ h(µ) sup µ (µ) (always) - erg. measures arb. dense periodic orbits (generic, Abdenur-Bonatti-Crovisier) sup µ (µ) = (f ) := sup O (f, O) - is continuous at generic diffeo - sup K h top (K) > (f ) ɛ open and dense
12 Application 4: Instability of the entropy M closed manifold with dim d 2, ω volume or symplectic form Let E 1 ω(m) := int({f Diff 1 ω(m) : no domination}) Theorem (B-Crovisier-Fisher) The topological entropy of a generic f E 1 ω(m) is equal to: (1) sup{h top (f, K) : K horseshoe} (2) sup{ (f, O) : O periodic orbit} (3) max 0<k<d lim n 1 n log sup E G k (TM) Jac(f n, E) Corollary h top is nowhere locally constant in E 1 ω(m) (robust instability) Corollary For any dense G δ G E 1 ω(m), h top (G) uncountable Corollary Generic f E 1 ω(m) is a continuity point of h top Diff 1 ω(m) Corollary C 1 generically : no domination h (f ) = h top (f )
13 Application 5: No mme and Borel classification M closed manifold with dim d 2, ω volume or symplectic form Theorem (B-Crovisier-Fisher) Generic f E 1 ω(m) has no measure maximizing the entropy Remark The diffeos with m.m.e. are dense (Newhouse theorem for C ) Combining horseshoes, no m.m.e. and Hochman (arxiv 2015): Corollary (B-C-F) There is dense G δ subset of E 1 ω(m) among which the topological entropy is a complete invariant for Borel conjugacy after removing periodic points
14 Proof of no m.m.e. - Concentration phenomenon f E 1 ω(m), dim M 2 Dynamical ball for x M, ɛ > 0: B f (x, ɛ, n) := {y M : 0 k < n d(f k y, f k x) < ɛ} Proposition 0 < ɛ, α < 1, for a dense set of f 0 E 1 ω(m), δ > 0, finite X M s.t. (*) if f close to f 0, µ P erg (f ), and h(f, µ) > h top (f ) δ, then µ( x X B f (x, ɛ, #X )) > 1 α Proof of Theorem. 1) G dense G δ E 1 ω(m) s.t. 0 < ɛ, α < 1 f G δ > 0 X finite satisfying (*) 2) Let f G, µ m.m.e., and ɛ > 0. From Katok s formula, need to bound: r f (µ, ɛ, n) := min{#c : µ( x C B f (x, ɛ, n)) > 1/2} 3) Take 0 < α << 1/ log min{#c : x C B(x, ɛ) = M}. Apply (*)
15 Conclusion Conjecture (higher smoothness) Given a C r -diffeo with hyperbolic periodic point p in a cycle of basic sets (see Gourmelon) with no dominated splitting, there is a C r -perturbation with a horseshoe with entropy (p)/r Question (internal perturbations) For a homoclinic class of a C 1 -generic diffeo, is the topological entropy the supremum of that of the horseshoes it contains? Question (entropy instability) Show that {f Diff 1 (M) : h top not locally constant at f } has non-empty interior Problem (entropy stability) Characterize the locus of entropy stability {U open in Diff 1 ω (M) : h top U = const} (Generically in Diff 1 ω (M): no domination h = h top) arxiv: , arxiv:1612:06914 JB, S. Crovisier, T. Fisher, The entropy of C 1 -diffeomorphisms without a dominated splitting JB, S. Crovisier, T. Fisher, Local perturbations of conservative C 1 diffeomorphisms
arxiv: v1 [math.ds] 6 Jun 2016
The entropy of C 1 -diffeomorphisms without a dominated splitting Jérôme Buzzi, Sylvain Crovisier, Todd Fisher arxiv:1606.01765v1 [math.ds] 6 Jun 2016 Tuesday 7 th June, 2016 Abstract A classical construction
More informationSymbolic extensions for partially hyperbolic diffeomorphisms
for partially hyperbolic diffeomorphisms Todd Fisher tfisher@math.byu.edu Department of Mathematics Brigham Young University Workshop on Partial Hyperbolicity Entropy Topological entropy measures the exponential
More informationSymbolic extensions for partially hyperbolic diffeomorphisms
for partially hyperbolic diffeomorphisms Todd Fisher tfisher@math.byu.edu Department of Mathematics Brigham Young University International Workshop on Global Dynamics Beyond Uniform Hyperbolicity Joint
More informationEssential hyperbolicity versus homoclinic bifurcations. Global dynamics beyond uniform hyperbolicity, Beijing 2009 Sylvain Crovisier - Enrique Pujals
Essential hyperbolicity versus homoclinic bifurcations Global dynamics beyond uniform hyperbolicity, Beijing 2009 Sylvain Crovisier - Enrique Pujals Generic dynamics Consider: M: compact boundaryless manifold,
More informationThe Structure of Hyperbolic Sets
The Structure of Hyperbolic Sets p. 1/35 The Structure of Hyperbolic Sets Todd Fisher tfisher@math.umd.edu Department of Mathematics University of Maryland, College Park The Structure of Hyperbolic Sets
More informationHyperbolic Dynamics. Todd Fisher. Department of Mathematics University of Maryland, College Park. Hyperbolic Dynamics p.
Hyperbolic Dynamics p. 1/36 Hyperbolic Dynamics Todd Fisher tfisher@math.umd.edu Department of Mathematics University of Maryland, College Park Hyperbolic Dynamics p. 2/36 What is a dynamical system? Phase
More informationMARKOV PARTITIONS FOR HYPERBOLIC SETS
MARKOV PARTITIONS FOR HYPERBOLIC SETS TODD FISHER, HIMAL RATHNAKUMARA Abstract. We show that if f is a diffeomorphism of a manifold to itself, Λ is a mixing (or transitive) hyperbolic set, and V is a neighborhood
More informationNonuniform hyperbolicity for C 1 -generic diffeomorphisms
Nonuniform hyperbolicity for C -generic diffeomorphisms Flavio Abdenur, Christian Bonatti, and Sylvain Crovisier September 8, 2008 Abstract We study the ergodic theory of non-conservative C -generic diffeomorphisms.
More informationPATH CONNECTEDNESS AND ENTROPY DENSITY OF THE SPACE OF HYPERBOLIC ERGODIC MEASURES
PATH CONNECTEDNESS AND ENTROPY DENSITY OF THE SPACE OF HYPERBOLIC ERGODIC MEASURES ANTON GORODETSKI AND YAKOV PESIN Abstract. We show that the space of hyperbolic ergodic measures of a given index supported
More informationSymbolic dynamics and non-uniform hyperbolicity
Symbolic dynamics and non-uniform hyperbolicity Yuri Lima UFC and Orsay June, 2017 Yuri Lima (UFC and Orsay) June, 2017 1 / 83 Lecture 1 Yuri Lima (UFC and Orsay) June, 2017 2 / 83 Part 1: Introduction
More informationSmooth Ergodic Theory and Nonuniformly Hyperbolic Dynamics
CHAPTER 2 Smooth Ergodic Theory and Nonuniformly Hyperbolic Dynamics Luis Barreira Departamento de Matemática, Instituto Superior Técnico, 1049-001 Lisboa, Portugal E-mail: barreira@math.ist.utl.pt url:
More informationA geometric approach for constructing SRB measures. measures in hyperbolic dynamics
A geometric approach for constructing SRB measures in hyperbolic dynamics Pennsylvania State University Conference on Current Trends in Dynamical Systems and the Mathematical Legacy of Rufus Bowen August
More informationHYPERBOLIC SETS WITH NONEMPTY INTERIOR
HYPERBOLIC SETS WITH NONEMPTY INTERIOR TODD FISHER, UNIVERSITY OF MARYLAND Abstract. In this paper we study hyperbolic sets with nonempty interior. We prove the folklore theorem that every transitive hyperbolic
More informationEquilibrium States for Partially Hyperbolic Horseshoes
Equilibrium States for Partially Hyperbolic Horseshoes R. Leplaideur, K. Oliveira, and I. Rios August 25, 2009 Abstract We study ergodic properties of invariant measures for the partially hyperbolic horseshoes,
More informationTOPOLOGICAL ENTROPY FOR DIFFERENTIABLE MAPS OF INTERVALS
Chung, Y-.M. Osaka J. Math. 38 (200), 2 TOPOLOGICAL ENTROPY FOR DIFFERENTIABLE MAPS OF INTERVALS YONG MOO CHUNG (Received February 9, 998) Let Á be a compact interval of the real line. For a continuous
More informationHomoclinic tangency and variation of entropy
CADERNOS DE MATEMÁTICA 10, 133 143 May (2009) ARTIGO NÚMERO SMA# 313 Homoclinic tangency and variation of entropy M. Bronzi * Departamento de Matemática, Instituto de Ciências Matemáticas e de Computação,
More informationSuper-exponential growth of the number of periodic orbits inside homoclinic classes p. 1/22
Super-exponential growth of the number of periodic orbits inside homoclinic classes p. 1/22 Super-exponential growth of the number of periodic orbits inside homoclinic classes Todd Fisher tfisher@math.umd.edu
More informationTRIVIAL CENTRALIZERS FOR AXIOM A DIFFEOMORPHISMS
TRIVIAL CENTRALIZERS FOR AXIOM A DIFFEOMORPHISMS TODD FISHER Abstract. We show there is a residual set of non-anosov C Axiom A diffeomorphisms with the no cycles property whose elements have trivial centralizer.
More informationarxiv: v1 [math.ds] 16 Nov 2010
Essential hyperbolicity and homoclinic bifurcations: a dichotomy phenomenon/mechanism for diffeomorphisms arxiv:1011.3836v1 [math.ds] 16 Nov 2010 Sylvain Crovisier Enrique R. Pujals October 30, 2018 Abstract
More informationThe Existence of Chaos in the Lorenz System
The Existence of Chaos in the Lorenz System Sheldon E. Newhouse Mathematics Department Michigan State University E. Lansing, MI 48864 joint with M. Berz, K. Makino, A. Wittig Physics, MSU Y. Zou, Math,
More information1 Introduction Definitons Markov... 2
Compact course notes Dynamic systems Fall 2011 Professor: Y. Kudryashov transcribed by: J. Lazovskis Independent University of Moscow December 23, 2011 Contents 1 Introduction 2 1.1 Definitons...............................................
More informationBOWEN S ENTROPY-CONJUGACY CONJECTURE IS TRUE UP TO FINITE INDEX
BOWEN S ENTROPY-CONJUGACY CONJECTURE IS TRUE UP TO FINITE INDEX MIKE BOYLE, JÉRÔME BUZZI, AND KEVIN MCGOFF Abstract. For a topological dynamical system (X, f), consisting of a continuous map f : X X, and
More informationEntropy in Dynamical Systems
Entropy in Dynamical Systems Lai-Sang Young In this article, the word entropy is used exclusively to refer to the entropy of a dynamical system, i.e. a map or a flow. It measures the rate of increase in
More informationPhysical measures of discretizations of generic diffeomorphisms
Ergod. Th. & Dynam. Sys. (2018), 38, 1422 1458 doi:10.1017/etds.2016.70 c Cambridge University Press, 2016 Physical measures of discretizations of generic diffeomorphisms PIERRE-ANTOINE GUIHÉNEUF Université
More informationPeriodic Sinks and Observable Chaos
Periodic Sinks and Observable Chaos Systems of Study: Let M = S 1 R. T a,b,l : M M is a three-parameter family of maps defined by where θ S 1, r R. θ 1 = a+θ +Lsin2πθ +r r 1 = br +blsin2πθ Outline of Contents:
More informationProblems in hyperbolic dynamics
Problems in hyperbolic dynamics Current Trends in Dynamical Systems and the Mathematical Legacy of Rufus Bowen Vancouver july 31st august 4th 2017 Notes by Y. Coudène, S. Crovisier and T. Fisher 1 Zeta
More informationUnique equilibrium states for geodesic flows in nonpositive curvature
Unique equilibrium states for geodesic flows in nonpositive curvature Todd Fisher Department of Mathematics Brigham Young University Fractal Geometry, Hyperbolic Dynamics and Thermodynamical Formalism
More informationTHE ENTROPY CONJECTURE FOR DIFFEOMORPHISMS AWAY FROM TANGENCIES
THE ENTROPY CONJECTURE FOR DIFFEOMORPHISMS AWAY FROM TANGENCIES GANG LIAO, MARCELO VIANA 2, JIAGANG YANG 3 Abstract. We prove that every C diffeomorphism away from homoclinic tangencies is entropy expansive,
More informationHyperbolic Sets That are Not Locally Maximal
Hyperbolic Sets That are Not Locally Maximal Todd Fisher December 6, 2004 Abstract This papers addresses the following topics relating to the structure of hyperbolic sets: First, hyperbolic sets that are
More informationApril 13, We now extend the structure of the horseshoe to more general kinds of invariant. x (v) λ n v.
April 3, 005 - Hyperbolic Sets We now extend the structure of the horseshoe to more general kinds of invariant sets. Let r, and let f D r (M) where M is a Riemannian manifold. A compact f invariant set
More informationHAMILTONIAN ELLIPTIC DYNAMICS ON SYMPLECTIC 4-MANIFOLDS
HAMILTONIAN ELLIPTIC DYNAMICS ON SYMPLECTIC 4-MANIFOLDS MÁRIO BESSA AND JOÃO LOPES DIAS Abstract. We consider C 2 Hamiltonian functions on compact 4-dimensional symplectic manifolds to study elliptic dynamics
More informationThe first half century of entropy: the most glorious number in dynamics
The first half century of entropy: the most glorious number in dynamics A. Katok Penn State University This is an expanded version of the invited talk given on June 17, 2003 in Moscow at the conference
More informationGeneric family with robustly infinitely many sinks
Generic family with robustly infinitely many sinks Pierre Berger November 6, 2018 arxiv:1411.6441v2 [math.ds] 10 Mar 2015 Abstract We show, for every r > d 0 or r = d 2, the existence of a Baire generic
More informationAbundance of stable ergodicity
Abundance of stable ergodicity Christian Bonatti, Carlos atheus, arcelo Viana, Amie Wilkinson December 7, 2002 Abstract We consider the set PH ω () of volume preserving partially hyperbolic diffeomorphisms
More informationOn the Structure of Hyperbolic Sets
NORTHWESTERN UNIVERSITY On the Structure of Hyperbolic Sets A DISSERTATION SUBMITTED TO THE GRADUATE SCHOOL IN PARTIAL FULFILLMENT OF THE REQUIREMENTS for the degree DOCTOR OF PHILOSOPHY Field of Mathematics
More informationVARIATIONAL PRINCIPLE FOR THE ENTROPY
VARIATIONAL PRINCIPLE FOR THE ENTROPY LUCIAN RADU. Metric entropy Let (X, B, µ a measure space and I a countable family of indices. Definition. We say that ξ = {C i : i I} B is a measurable partition if:
More informationIntroduction Hyperbolic systems Beyond hyperbolicity Counter-examples. Physical measures. Marcelo Viana. IMPA - Rio de Janeiro
IMPA - Rio de Janeiro Asymptotic behavior General observations A special case General problem Let us consider smooth transformations f : M M on some (compact) manifold M. Analogous considerations apply
More informationGeneric family with robustly infinitely many sinks
Generic family with robustly infinitely many sinks Pierre Berger February 28, 2019 arxiv:1411.6441v1 [math.ds] 24 Nov 2014 Abstract We show, for every r > d 0 or r = d 2, the existence of a Baire generic
More informationarxiv: v1 [math.ds] 19 Jan 2017
A robustly transitive diffeomorphism of Kan s type CHENG CHENG, SHAOBO GAN AND YI SHI January 2, 217 arxiv:171.5282v1 [math.ds] 19 Jan 217 Abstract We construct a family of partially hyperbolic skew-product
More informationENTROPY-EXPANSIVENESS FOR PARTIALLY HYPERBOLIC DIFFEOMORPHISMS.
ENTROPY-EXPANSIVENESS FOR PARTIALLY HYPERBOLIC DIFFEOMORPHISMS. L. J. DÍAZ, T. FISHER, M. J. PACIFICO, AND J. L. VIEITEZ Abstract. We show that diffeomorphisms with a dominated splitting of the form E
More informationA non-uniform Bowen s equation and connections to multifractal analysis
A non-uniform Bowen s equation and connections to multifractal analysis Vaughn Climenhaga Penn State November 1, 2009 1 Introduction and classical results Hausdorff dimension via local dimensional characteristics
More informationRobustly transitive diffeomorphisms
Robustly transitive diffeomorphisms Todd Fisher tfisher@math.byu.edu Department of Mathematics, Brigham Young University Summer School, Chengdu, China 2009 Dynamical systems The setting for a dynamical
More informationCoexistence of Zero and Nonzero Lyapunov Exponents
Coexistence of Zero and Nonzero Lyapunov Exponents Jianyu Chen Pennsylvania State University July 13, 2011 Outline Notions and Background Hyperbolicity Coexistence Construction of M 5 Construction of the
More informationSYMBOLIC DYNAMICS FOR HYPERBOLIC SYSTEMS. 1. Introduction (30min) We want to find simple models for uniformly hyperbolic systems, such as for:
SYMBOLIC DYNAMICS FOR HYPERBOLIC SYSTEMS YURI LIMA 1. Introduction (30min) We want to find simple models for uniformly hyperbolic systems, such as for: [ ] 2 1 Hyperbolic toral automorphisms, e.g. f A
More informationA FRANKS LEMMA FOR CONVEX PLANAR BILLIARDS
A FRANKS LEMMA FOR CONVEX PLANAR BILLIARDS DANIEL VISSCHER Abstract Let γ be an orbit of the billiard flow on a convex planar billiard table; then the perpendicular part of the derivative of the billiard
More informationOPEN PROBLEMS IN THE THEORY OF NON-UNIFORM HYPERBOLICITY
OPEN PROBLEMS IN THE THEORY OF NON-UNIFORM HYPERBOLICITY YAKOV PESIN AND VAUGHN CLIMENHAGA Abstract. This is a survey-type article whose goal is to review some recent developments in studying the genericity
More informationWHAT IS A CHAOTIC ATTRACTOR?
WHAT IS A CHAOTIC ATTRACTOR? CLARK ROBINSON Abstract. Devaney gave a mathematical definition of the term chaos, which had earlier been introduced by Yorke. We discuss issues involved in choosing the properties
More informationHYPERBOLICITY AND RECURRENCE IN DYNAMICAL SYSTEMS: A SURVEY OF RECENT RESULTS
HYPERBOLICITY AND RECURRENCE IN DYNAMICAL SYSTEMS: A SURVEY OF RECENT RESULTS LUIS BARREIRA Abstract. We discuss selected topics of current research interest in the theory of dynamical systems, with emphasis
More informationAbundance of stable ergodicity
Abundance of stable ergodicity Christian Bonatti, Carlos Matheus, Marcelo Viana, Amie Wilkinson October 5, 2004 Abstract We consider the set PH ω (M) of volume preserving partially hyperbolic diffeomorphisms
More informationPARTIAL HYPERBOLICITY, LYAPUNOV EXPONENTS AND STABLE ERGODICITY
PARTIAL HYPERBOLICITY, LYAPUNOV EXPONENTS AND STABLE ERGODICITY K. BURNS, D. DOLGOPYAT, YA. PESIN Abstract. We present some results and open problems about stable ergodicity of partially hyperbolic diffeomorphisms
More informationOn the smoothness of the conjugacy between circle maps with a break
On the smoothness of the conjugacy between circle maps with a break Konstantin Khanin and Saša Kocić 2 Department of Mathematics, University of Toronto, Toronto, ON, Canada M5S 2E4 2 Department of Mathematics,
More informationAdapted metrics for dominated splittings
Adapted metrics for dominated splittings Nikolaz Gourmelon January 15, 27 Abstract A Riemannian metric is adapted to an hyperbolic set of a diffeomorphism if, in this metric, the expansion/contraction
More informationLyapunov optimizing measures for C 1 expanding maps of the circle
Lyapunov optimizing measures for C 1 expanding maps of the circle Oliver Jenkinson and Ian D. Morris Abstract. For a generic C 1 expanding map of the circle, the Lyapunov maximizing measure is unique,
More informationUniversity of York. Extremality and dynamically defined measures. David Simmons. Diophantine preliminaries. First results. Main results.
University of York 1 2 3 4 Quasi-decaying References T. Das, L. Fishman, D. S., M. Urbański,, I: properties of quasi-decaying, http://arxiv.org/abs/1504.04778, preprint 2015.,, II: Measures from conformal
More informationGEOMETRIC PRESSURE FOR MULTIMODAL MAPS OF THE INTERVAL
GEOMETRIC PRESSURE FOR MULTIMODAL MAPS OF THE INTERVAL FELIKS PRZYTYCKI AND JUAN RIVERA-LETELIER Abstract. This paper is an interval dynamics counterpart of three theories founded earlier by the authors,
More informationThermodynamics for discontinuous maps and potentials
Thermodynamics for discontinuous maps and potentials Vaughn Climenhaga University of Houston July 11, 2013 Plan of talk Dynamical system { X a complete separable metric space f : X X a measurable map Potential
More informationA stochastic view of Dynamical Systems
A stochastic view ofdynamical Systems p. 1/1 A stochastic view of Dynamical Systems Marcelo Viana IMPA - Rio de Janeiro A stochastic view ofdynamical Systems p. 2/1 Dynamical systems Transformations or
More informationA Complex Gap Lemma. Sébastien Biebler
A Complex Gap Lemma Sébastien Biebler arxiv:80.0544v [math.ds] 5 Oct 08 Abstract Inspired by the work of Newhouse in one real variable, we introduce a relevant notion of thickness for dynamical Cantor
More informationSTABLE ERGODICITY FOR PARTIALLY HYPERBOLIC ATTRACTORS WITH NEGATIVE CENTRAL EXPONENTS
STABLE ERGODICITY FOR PARTIALLY HYPERBOLIC ATTRACTORS WITH NEGATIVE CENTRAL EXPONENTS K. BURNS, D. DOLGOPYAT, YA. PESIN, M. POLLICOTT Dedicated to G. A. Margulis on the occasion of his 60th birthday Abstract.
More informationMañé s Conjecture from the control viewpoint
Mañé s Conjecture from the control viewpoint Université de Nice - Sophia Antipolis Setting Let M be a smooth compact manifold of dimension n 2 be fixed. Let H : T M R be a Hamiltonian of class C k, with
More informationQuantum ergodicity. Nalini Anantharaman. 22 août Université de Strasbourg
Quantum ergodicity Nalini Anantharaman Université de Strasbourg 22 août 2016 I. Quantum ergodicity on manifolds. II. QE on (discrete) graphs : regular graphs. III. QE on graphs : other models, perspectives.
More informationON HYPERBOLIC MEASURES AND PERIODIC ORBITS
ON HYPERBOLIC MEASURES AND PERIODIC ORBITS ILIE UGARCOVICI Dedicated to Anatole Katok on the occasion of his 60th birthday Abstract. We prove that if a diffeomorphism on a compact manifold preserves a
More informationLipschitz shadowing implies structural stability
Lipschitz shadowing implies structural stability Sergei Yu. Pilyugin Sergei B. Tihomirov Abstract We show that the Lipschitz shadowing property of a diffeomorphism is equivalent to structural stability.
More informationTopological Properties of Invariant Sets for Anosov Maps with Holes
Brigham Young University BYU ScholarsArchive All Theses and Dissertations 2011-11-10 Topological Properties of Invariant Sets for Anosov Maps with Holes Skyler C. Simmons Brigham Young University - Provo
More informationLecture 5: Oscillatory motions for the RPE3BP
Lecture 5: Oscillatory motions for the RPE3BP Marcel Guardia Universitat Politècnica de Catalunya February 10, 2017 M. Guardia (UPC) Lecture 5 February 10, 2017 1 / 25 Outline Oscillatory motions for the
More informationOn dynamical properties of multidimensional diffeomorphisms from Newhouse regions: I
IOP PUBLISHING Nonlinearity 2 (28) 923 972 NONLINEARITY doi:.88/95-775/2/5/3 On dynamical properties of multidimensional diffeomorphisms from Newhouse regions: I S V Gonchenko, L P Shilnikov and D V Turaev
More informationPOINTWISE DIMENSION AND ERGODIC DECOMPOSITIONS
POINTWISE DIMENSION AND ERGODIC DECOMPOSITIONS LUIS BARREIRA AND CHRISTIAN WOLF Abstract. We study the Hausdorff dimension and the pointwise dimension of measures that are not necessarily ergodic. In particular,
More informationCENTER LYAPUNOV EXPONENTS IN PARTIALLY HYPERBOLIC DYNAMICS
CENTER LYAPUNOV EXPONENTS IN PARTIALLY HYPERBOLIC DYNAMICS ANDREY GOGOLEV AND ALI TAHZIBI Contents 1. Introduction 2 2. Abundance of non-zero Lyapunov exponents 3 2.1. Removing zero exponent for smooth
More informationDynamics of Group Actions and Minimal Sets
University of Illinois at Chicago www.math.uic.edu/ hurder First Joint Meeting of the Sociedad de Matemática de Chile American Mathematical Society Special Session on Group Actions: Probability and Dynamics
More informationSUPER-EXPONENTIAL GROWTH OF THE NUMBER OF PERIODIC ORBITS INSIDE HOMOCLINIC CLASSES. Aim Sciences. (Communicated by Aim Sciences)
Manuscript submitted to AIMS Journals Volume X, Number 0X, XX 200X Website: http://aimsciences.org pp. X XX SUPER-EXPONENTIAL GROWTH OF THE NUMBER OF PERIODIC ORBITS INSIDE HOMOCLINIC CLASSES Aim Sciences
More informationTECHNIQUES FOR ESTABLISHING DOMINATED SPLITTINGS
TECHNIQUES FOR ESTABLISHING DOMINATED SPLITTINGS ANDY HAMMERLINDL ABSTRACT. We give theorems which establish the existence of a dominated splitting and further properties, such as partial hyperbolicity.
More informationLOCAL ENTROPY THEORY
LOCAL ENTROPY THEORY ELI GLASNER AND XIANGDONG YE Abstract. In this survey we offer an overview of the so called local entropy theory, developed since the early 1990s. While doing so we emphasize the connections
More informationDIFFEOMORPHISMS WITH POSITIVE METRIC ENTROPY
DIFFEOMORPHISMS WITH POSITIVE METRIC ENTROPY A. AVILA, S. CROVISIER, AND A. WILKINSON Abstract. We obtain a dichotomy for C -generic, volume-preserving diffeomorphisms: either all the Lyapunov exponents
More informationDIMENSION ESTIMATES FOR NON-CONFORMAL REPELLERS AND CONTINUITY OF SUB-ADDITIVE TOPOLOGICAL PRESSURE
DIMENSION ESTIMATES FOR NON-CONFORMAL REPELLERS AND CONTINUITY OF SUB-ADDITIVE TOPOLOGICAL PRESSURE YONGLUO CAO, YAKOV PESIN, AND YUN ZHAO Abstract. Given a non-conformal repeller Λ of a C +γ map, we study
More informationMINIMAL YET MEASURABLE FOLIATIONS
MINIMAL YET MEASURABLE FOLIATIONS G. PONCE, A. TAHZIBI, AND R. VARÃO Abstract. In this paper we mainly address the problem of disintegration of Lebesgue measure along the central foliation of volume preserving
More information2. Hyperbolic dynamical systems
2. Hyperbolic dynamical systems The next great era of awakening of human intellect may well produce a method of understanding the qualitative content of equations. Today we cannot. Today we cannot see
More informationUNIQUE EQUILIBRIUM STATES FOR THE ROBUSTLY TRANSITIVE DIFFEOMORPHISMS OF
UNIQUE EQUILIBRIUM STATES FOR THE ROBUSTLY TRANSITIVE DIFFEOMORPHISMS OF MAÑÉ AND BONATTI VIANA VAUGHN CLIMENHAGA, TODD FISHER, AND DANIEL J. THOMPSON Abstract. We show that the families of robustly transitive
More informationHausdorff dimension for horseshoes
Ergod. Th. & Dyam. Sys. (1983), 3, 251-260 Printed in Great Britain Hausdorff dimension for horseshoes HEATHER McCLUSKEY AND ANTHONY MANNING Mathematics Institute, University of Warwick, Coventry CVA 1AL,
More informationPersistent Chaos in High-Dimensional Neural Networks
Persistent Chaos in High-Dimensional Neural Networks D. J. Albers with J. C. Sprott and James P. Crutchfield February 20, 2005 1 Outline: Introduction and motivation Mathematical versus computational dynamics
More informationPHY411 Lecture notes Part 5
PHY411 Lecture notes Part 5 Alice Quillen January 27, 2016 Contents 0.1 Introduction.................................... 1 1 Symbolic Dynamics 2 1.1 The Shift map.................................. 3 1.2
More informationIntroduction to Continuous Dynamical Systems
Lecture Notes on Introduction to Continuous Dynamical Systems Fall, 2012 Lee, Keonhee Department of Mathematics Chungnam National Univeristy - 1 - Chap 0. Introduction What is a dynamical system? A dynamical
More informationABSOLUTE CONTINUITY OF FOLIATIONS
ABSOLUTE CONTINUITY OF FOLIATIONS C. PUGH, M. VIANA, A. WILKINSON 1. Introduction In what follows, U is an open neighborhood in a compact Riemannian manifold M, and F is a local foliation of U. By this
More informationTOPOLOGICAL STRUCTURE OF PARTIALLY HYPERBOLIC ATTRACTORS. José F. Alves
TOPOLOGICAL STRUCTURE OF PARTIALLY HYPERBOLIC ATTRACTORS by José F. Alves Contents Introduction............................................................ 2 1. Partially hyperbolic sets..............................................
More informationContinuum-Wise Expansive and Dominated Splitting
Int. Journal of Math. Analysis, Vol. 7, 2013, no. 23, 1149-1154 HIKARI Ltd, www.m-hikari.com Continuum-Wise Expansive and Dominated Splitting Manseob Lee Department of Mathematics Mokwon University Daejeon,
More informationDYNAMICAL SYSTEMS. I Clark: Robinson. Stability, Symbolic Dynamics, and Chaos. CRC Press Boca Raton Ann Arbor London Tokyo
DYNAMICAL SYSTEMS Stability, Symbolic Dynamics, and Chaos I Clark: Robinson CRC Press Boca Raton Ann Arbor London Tokyo Contents Chapter I. Introduction 1 1.1 Population Growth Models, One Population 2
More information4 Countability axioms
4 COUNTABILITY AXIOMS 4 Countability axioms Definition 4.1. Let X be a topological space X is said to be first countable if for any x X, there is a countable basis for the neighborhoods of x. X is said
More informationThe Zorich Kontsevich Conjecture
The Zorich Kontsevich Conjecture Marcelo Viana (joint with Artur Avila) IMPA - Rio de Janeiro The Zorich Kontsevich Conjecture p.1/27 Translation Surfaces Compact Riemann surface endowed with a non-vanishing
More informationC 1 DENSITY OF AXIOM A FOR 1D DYNAMICS
C 1 DENSITY OF AXIOM A FOR 1D DYNAMICS DAVID DIICA Abstract. We outline a proof of the C 1 unimodal maps of the interval. density of Axiom A systems among the set of 1. Introduction The amazing theory
More informationProblem Set 2: Solutions Math 201A: Fall 2016
Problem Set 2: s Math 201A: Fall 2016 Problem 1. (a) Prove that a closed subset of a complete metric space is complete. (b) Prove that a closed subset of a compact metric space is compact. (c) Prove that
More informationDYNAMICAL SYSTEMS PROBLEMS. asgor/ (1) Which of the following maps are topologically transitive (minimal,
DYNAMICAL SYSTEMS PROBLEMS http://www.math.uci.edu/ asgor/ (1) Which of the following maps are topologically transitive (minimal, topologically mixing)? identity map on a circle; irrational rotation of
More informationThe centralizer of a C 1 generic diffeomorphism is trivial
The centralizer of a C 1 generic diffeomorphism is trivial Christian Bonatti, Sylvain Crovisier and Amie Wilkinson April 16, 2008 Abstract Answering a question of Smale, we prove that the space of C 1
More informationTHE GEOMETRIC APPROACH FOR CONSTRUCTING SINAI-RUELLE-BOWEN MEASURES
THE GEOMETRIC APPROACH FOR CONSTRUCTING SINAI-RUELLE-BOWEN MEASURES VAUGHN CLIMENHAGA, STEFANO LUZZATTO, AND YAKOV PESIN Abstract. An important class of physically relevant measures for dynamical systems
More informationLecture 4. Entropy and Markov Chains
preliminary version : Not for diffusion Lecture 4. Entropy and Markov Chains The most important numerical invariant related to the orbit growth in topological dynamical systems is topological entropy.
More informationSRB MEASURES FOR AXIOM A ENDOMORPHISMS
SRB MEASURES FOR AXIOM A ENDOMORPHISMS MARIUSZ URBANSKI AND CHRISTIAN WOLF Abstract. Let Λ be a basic set of an Axiom A endomorphism on n- dimensional compact Riemannian manifold. In this paper, we provide
More informationORBITAL SHADOWING, INTERNAL CHAIN TRANSITIVITY
ORBITAL SHADOWING, INTERNAL CHAIN TRANSITIVITY AND ω-limit SETS CHRIS GOOD AND JONATHAN MEDDAUGH Abstract. Let f : X X be a continuous map on a compact metric space, let ω f be the collection of ω-limit
More informationPhysical Measures. Stefano Luzzatto Abdus Salam International Centre for Theoretical Physics Trieste, Italy.
Physical Measures Stefano Luzzatto Abdus Salam International Centre for Theoretical Physics Trieste, Italy. International conference on Dynamical Systems Hammamet, Tunisia September 5-7, 2017 Let f : M
More informationNonlocally Maximal Hyperbolic Sets for Flows
Brigham Young University BYU ScholarsArchive All Theses and Dissertations 2015-06-01 Nonlocally Maximal Hyperbolic Sets for Flows Taylor Michael Petty Brigham Young University - Provo Follow this and additional
More informationPreprint Preprint Preprint Preprint
CADERNOS DE MATEMÁTICA 16, 179 187 May (2015) ARTIGO NÚMERO SMA#12 Regularity of invariant foliations and its relation to the dynamics R. Varão * Departamento de Matemática, Instituto de Matemática, Estatística
More informationSmooth flows with fractional entropy dimension
Smooth flows with fractional entropy dimension Steve Hurder MCA Montreal, July 27, 2017 University of Illinois at Chicago www.math.uic.edu/ hurder Theorem (K. Kuperberg, 1994) Let M be a closed, orientable
More information