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MATH34042: Discrete Time Dynamical Systems David Broomhead (Based on Original Notes by James Montaldi) School of Mathematics, University of Manchester 2008/9
MATH34042: Discrete Time Dynamical Systems David Broomhead (based on original notes by James Montaldi) School of Mathematics, University of Manchester 2008/9 Webpage: http://www.maths.manchester.ac.uk/∼dsb/Teaching/DynSys email: [email protected] Overview (2 lectures) Dynamical systems continuous/discrete; autonomous/non-autonomous. Iteration, orbit. Applica- tions (population dynamics, Newton’s method). A dynamical system is a map f : S S, and the set S is called the state space. Given an initial point x0 S, the orbit of x0 is the sequence x0,x1,x2,x3,... obtained by repeatedly applying f: ∈ → n x1 = f(x0), x2 = f(x1), x3 = f(x2),...,xn = f (x0), ... Basic question of dynamical systems: given x0, what is behaviour of orbit? Or, what is behaviour of most orbits? + + Example Let f : R R be given by f(x)= √x. Let x0 = 2. Then x1 = f(2)= √2 1.4142. And ≈ x = √2 1.1892 and x = √1.1892 1.0905. 2 p → 3 The orbit of≈2 therefore begins {2.0, 1.4142,≈ 1.1892, 1.0905, ...}. The orbit of 3 begins {3.0, 1.7321, 1.3161, 1.1472, ...}. The orbit of 0.5 begins {0.5, 0.7071, 0.8409, .9170, .9576, ...}. All are getting closer to 1. Regular dynamics fixed points, periodic points and orbits. Example f(x)= cos(x). Globally attracting fixed point at x = 0.739085 . ··· Chaotic dynamics Basic idea is unpredictability. There is no “typical’ behaviour. Example f(x)= 4x(1 − x), x [0,1]: Split the interval into two halves: L = [0, 1 ] and R = [ 1 ,1]. -
On the Combinatorics of External Rays in the Dynamics of the Complex Henon
ON THE COMBINATORICS OF EXTERNAL RAYS IN THE DYNAMICS OF THE COMPLEX HENON MAP. A Dissertation Presented to the Faculty of the Graduate School of Cornell University in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy by Ricardo Antonio Oliva May 1998 c Ricardo Antonio Oliva 1998 ALL RIGHTS RESERVED Addendum. This is a slightly revised version of my doctoral thesis: some typing and spelling mistakes have been corrected and a few sentences have been re-worded for better legibility (particularly in section 4.3). Also, to create a nicer pdf document with hyperref, the title of section 3.3.2 has been made shorter. The original title was A model for a map with an attracting fixed point as well as a period-3 sink: the (3-1)-graph. ON THE COMBINATORICS OF EXTERNAL RAYS IN THE DYNAMICS OF THE COMPLEX HENON MAP. Ricardo Antonio Oliva , Ph.D. Cornell University 1998 We present combinatorial models that describe quotients of the solenoid arising from the dynamics of the complex H´enon map 2 2 2 fa,c : C → C , (x, y) → (x + c − ay, x). These models encode identifications of external rays for specific mappings in the H´enon family. We investigate the structure of a region of parameter space in R2 empirically, using computational tools we developed for this study. We give a combi- natorial description of bifurcations arising from changes in the set of identifications of external rays. Our techniques enable us to detect, predict, and locate bifurca- tion curves in parameter space. We describe a specific family of bifurcations in a region of real parameter space for which the mappings were expected to have sim- ple dynamics. -
Efficient Method for Detection of Periodic Orbits in Chaotic Maps And
Efficient Method for Detection of Periodic Orbits in Chaotic Maps and Flows A Thesis by Jonathan Crofts in partial fulfillment of the requirements for the degree of Doctor of Philosophy. Department of Mathematics University of Leicester March 2007. c Jonathan J Crofts, 2007. arXiv:0706.1940v2 [nlin.CD] 13 Jun 2007 Acknowledgements I would like to thank Ruslan Davidchack, my supervisor, for his many suggestions and constant support and understanding during this research. I am also thankful to Michael Tretyakov for his support and advice. Further, I would like to acknowledge my gratitude to the people from the Department of Mathematics at the University of Leicester for their help and support. Finally, I would like to thank my family and friends for their patience and sup- port throughout the past few years. In particular, I thank my wife Lisa and my daughter Ellen, without whom I would have completed this research far quicker, but somehow, it just would not have been the same. At this point I would also like to reassure Lisa that I will get a real job soon. Leicester, Leicestershire, UK Jonathan J. Crofts 31 March 2007 i Contents Abstract iv List of figures v List of tables vi 1 Introduction 1 1.1 History,theoryandapplications . 1 1.2 Periodicorbits............................... 3 1.2.1 Periodicorbittheory . 4 1.2.2 Efficient detection of UPOs . 6 1.3 Extendedsystems............................. 9 1.4 Anoteonnumerics............................ 10 1.4.1 Intervalarithmetic . 12 1.5 Overview.................................. 14 1.6 Thesisresults ............................... 16 2 Conventional techniques for detecting periodic orbits 18 2.1 Specialcases................................ 18 2.1.1 One-dimensionalmaps . -
Infinitely Renormalizable Quadratic Polynomials 1
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 352, Number 11, Pages 5077{5091 S 0002-9947(00)02514-9 Article electronically published on July 12, 2000 INFINITELY RENORMALIZABLE QUADRATIC POLYNOMIALS YUNPING JIANG Abstract. We prove that the Julia set of a quadratic polynomial which ad- mits an infinite sequence of unbranched, simple renormalizations with complex bounds is locally connected. The method in this study is three-dimensional puzzles. 1. Introduction Let P (z)=z2 + c be a quadratic polynomial where z is a complex variable and c is a complex parameter. The filled-in Julia set K of P is, by definition, the set of points z which remain bounded under iterations of P .TheJulia set J of P is the boundary of K. A central problem in the study of the dynamical system generated by P is to understand the topology of a Julia set J, in particular, the local connectivity for a connected Julia set. A connected set J in the complex plane is said to be locally connected if for every point p in J and every neighborhood U of p there is a neighborhood V ⊆ U such that V \ J is connected. We first give the definition of renormalizability. A quadratic-like map F : U ! V is a holomorphic, proper, degree two branched cover map, whereT U and V are ⊂ 1 −n two domains isomorphic to a disc and U V .ThenKF = n=0 F (U)and JF = @KF are the filled-in Julia set and the Julia set of F , respectively. We only consider those quadratic-like maps whose Julia sets are connected. -
Geography of the Cubic Connectedness Locus : Intertwining Surgery
ANNALES SCIENTIFIQUES DE L’É.N.S. ADAM EPSTEIN MICHAEL YAMPOLSKY Geography of the cubic connectedness locus : intertwining surgery Annales scientifiques de l’É.N.S. 4e série, tome 32, no 2 (1999), p. 151-185 <http://www.numdam.org/item?id=ASENS_1999_4_32_2_151_0> © Gauthier-Villars (Éditions scientifiques et médicales Elsevier), 1999, tous droits réservés. L’accès aux archives de la revue « Annales scientifiques de l’É.N.S. » (http://www. elsevier.com/locate/ansens) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systé- matique est constitutive d’une infraction pénale. Toute copie ou impression de ce fi- chier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. sclent. EC. Norm. Sup., 4e serie, t 32, 1999, p. 151 a 185. GEOGRAPHY OF THE CUBIC CONNECTEDNESS LOCUS: INTERTWINING SURGERY BY ADAM EPSTEIN AND MICHAEL YAMPOLSKY ABSTRACT. - We exhibit products of Mandelbrot sets in the two-dimensional complex parameter space of cubic polynomials. Cubic polynomials in such a product may be renormalized to produce a pair of quadratic maps. The inverse construction intertwining two quadratics is realized by means of quasiconformal surgery. The associated asymptotic geography of the cubic connectedness locus is discussed in the Appendix. © Elsevier, Paris RESUME. - Nous trouvons des produits de Fensemble de Mandelbrot dans 1'espace a deux variables complexes des polynomes cubiques. La renormalisation d'un polyn6me cubique appartenant a un tel produit donne deux polyn6mes quadratiques. Le precede inverse qui entrelace deux polynomes quadratiques est obtenu par chirurgie quasiconforme. -
1D Dynamics: Symbolic Coding
1D Dynamics: Symbolic Coding 1. Full shift of two symbols – Let X = {s =(s0s1s2 ··· si ··· ); si =0 or 1} be the collection of all sequences of 0 and 1. – For s =(s0s1 ··· si ··· ), t =(t0t1 ··· ti ··· ), let ∞ |s − t | d(s, t) = i i X i i=0 2 Claim: (i) (X,d) is a metric space. s t 1 (ii) d( , ) ≤ 2n iff si = ti for all i < n. Proof: (i) d(s, t) ≥ 0 and d(s, t) = d(t, s) are obvious. For the triangle inequality, observe ∞ ∞ ∞ |si − ti| |si − vi| |vi − ti| d(s, t) = ≤ + X 2i X 2i X 2i i=0 i=0 i=0 = d(s, v)+ d(v, t). (ii) is straight forward from definition. – Let σ : X → X be define by σ(s0s1 ··· si ··· )=(s1s2 ··· si+1 ··· ). Claim: σ : X → X is continuous. Proof: 1 For ε > 0 given let n be such that 2n < ε. Let 1 s t s t δ = 2n+1 . For d( , ) <δ, d(σ( ), σ( )) < ε. – (X,σ) as a dynamical system: Claim (a) σ : X → X have exactly 2n periodic points of period n. (b) Union of all periodic orbits are dense in X. (c) There exists a transitive orbit. Proof: (a) The number of periodic point in X is the same as the number of strings of 0, 1 of length n, which is 2n. (b) ∀s =(s0s1 · · · sn · · · ), let sn =(s0s1 · · · sn; s0s1 · · · sn; · · · ). We have 1 d(sn, s) < . 2n−1 So sn → s as n →∞. (c) List all possible strings of length 1, then of length 2, then of length 3, and so on. -
Multiple Periodic Solutions and Fractal Attractors of Differential Equations with N-Valued Impulses
mathematics Article Multiple Periodic Solutions and Fractal Attractors of Differential Equations with n-Valued Impulses Jan Andres Department of Mathematical Analysis and Applications of Mathematics, Faculty of Science, Palacký University, 17. listopadu 12, 771 46 Olomouc, Czech Republic; [email protected] Received: 10 September 2020; Accepted: 30 September 2020; Published: 3 October 2020 Abstract: Ordinary differential equations with n-valued impulses are examined via the associated Poincaré translation operators from three perspectives: (i) the lower estimate of the number of periodic solutions on the compact subsets of Euclidean spaces and, in particular, on tori; (ii) weakly locally stable (i.e., non-ejective in the sense of Browder) invariant sets; (iii) fractal attractors determined implicitly by the generating vector fields, jointly with Devaney’s chaos on these attractors of the related shift dynamical systems. For (i), the multiplicity criteria can be effectively expressed in terms of the Nielsen numbers of the impulsive maps. For (ii) and (iii), the invariant sets and attractors can be obtained as the fixed points of topologically conjugated operators to induced impulsive maps in the hyperspaces of the compact subsets of the original basic spaces, endowed with the Hausdorff metric. Five illustrative examples of the main theorems are supplied about multiple periodic solutions (Examples 1–3) and fractal attractors (Examples 4 and 5). Keywords: impulsive differential equations; n-valued maps; Hutchinson-Barnsley operators; multiple periodic solutions; topological fractals; Devaney’s chaos on attractors; Poincaré operators; Nielsen number MSC: 28A20; 34B37; 34C28; Secondary 34C25; 37C25; 58C06 1. Introduction The theory of impulsive differential equations and inclusions has been systematically developed (see e.g., the monographs [1–4], and the references therein), among other things, especially because of many practical applications (see e.g., References [1,4–11]). -
The External Boundary of the Bifurcation Locus M2 1
THE EXTERNAL BOUNDARY OF THE BIFURCATION LOCUS M2 V. TIMORIN Abstract. Consider a quadratic rational self-map of the Riemann sphere such that one critical point is periodic of period 2, and the other critical point lies on the boundary of its immediate basin of attraction. We will give explicit topological models for all such maps. We also discuss the corresponding parameter picture. 1. Introduction 1.1. The family V2. Consider the set V2 of holomorphic conjugacy classes of qua- dratic rational maps that have a super-attracting periodic cycle of period 2 (we follow the notation of Mary Rees). The complement in V2 to the class of the single map z 1/z2 is denoted by V . The set V is parameterized by a single com- 7→ 2,0 2,0 plex number. Indeed, for any map f in V2,0, the critical point of period two can be mapped to , its f-image to 0, and the other critical point to 1. Then we obtain a map of the∞ form − a f (z)= , a = 0 a z2 + 2z 6 holomorphically conjugate to f. Thus the set V is identified with C 0. 2,0 − The family V2 is just the second term in the sequence V1, V2, V3,... , where, by def- inition, Vn consists of holomorphic conjugacy classes of quadratic rational maps with a periodic critical orbit of period n. Such maps have one “free” critical point, hence each family Vn has complex dimension 1. Note that V1 is the family of quadratic polynomials, i.e., holomorphic endomorphisms of the Riemann sphere of degree 2 with a fixed critical point at . -
Bifurcation in Complex Quadrat Ic Polynomial and Some Folk Theorems Involving the Geometry of Bulbs of the Mandelbrot Set
Bifurcation in Complex Quadrat ic Polynomial and Some Folk Theorems Involving the Geometry of Bulbs of the Mandelbrot Set Monzu Ara Begum A Thesis in The Department of Mat hemat ics and St at ist ics Presented in Partial F'uffilment of the Requirements for the Degree of Master of Science at Concordia University Montreal, Quebec, Canada May 2001 @Monzu Ara Begum, 2001 muisitions and Acquisitions et BiMiiriic Services senrices bibliographiques The author has granted a non- L'auteur a accordé une licence non exclusive licence aiiowing the exclusive permettant à la National Li'brary of Caoada to Bibliothèque nationale du Canada de reproduce, loan, distribute or seiî reproduire, prêtex' distribuer ou copies of this thesis in microform, vendre des copies de cette thèse sous paper or electronic formats. la forme de micmfiche/nlm. de reproduction sur papier ou sur format électronique. The auîhor retains ownership of the L'auteur conserve la propriété du copyright in this thesis. Neither the droit d'auteur qui protège cette thèse. thesis nor substantial extracts fiom it Ni La îhèse ni des extraits substantiels may be printed or otherwise de celle-ci ne doivent être imprimés reproduced without the author's ou autrement reproduits sans son permission. autorisation. Abstract Bifurcation in Complex Quadratic Polynomial and Some Folk Theorems Involving the Geometry of Bulbs of the Mandelbrot Set Monzu Ara Begum The Mandelbrot set M is a subset of the parameter plane for iteration of the complex quadratic polynomial Q,(z) = z2 +c. M consists of those c values for which the orbit of O is bounded. -
Sharkovsky's Ordering and Chaos Introduction to Fractal Geometry and Chaos
Sharkovsky's Ordering and Chaos Introduction to Fractal Geometry and Chaos Matilde Marcolli MAT1845HS Winter 2020, University of Toronto M 1-2 and T 10-12 BA6180 Sharkovsky's Ordering and Chaos Introduction to Fractal Geometry and Chaos Matilde Marcolli References for this lecture: K. Burns and B. Hasselblatt, The Sharkovsky theorem: a natural direct proof, Amer. Math. Monthly 118 (2011), no. 3, 229{244 T.Y.Li and A.Yorke, Period three implies chaos, The American Mathematical Monthly, Vol. 82, No. 10. (Dec., 1975) 985{992 O.M. Sharkovsky, Co-existence of cycles of a continuous mapping of the line into itself, Ukrain. Mat. Z. 16 (1964) 61{71 B. Luque, L. Lacasa, F.J. Ballesteros, A. Robledo, Feigenbaum Graphs: A Complex Network Perspective of Chaos, PLoS ONE 6(9): e2241 L. Alsed`a,J. Llibre, M. Misiurewicz, Combinatorial dynamics and entropy in dimension one, World Scientific, 2000 Sharkovsky's Ordering and Chaos Introduction to Fractal Geometry and Chaos Matilde Marcolli Period 3 implies Chaos • T.Y.Li and A.Yorke, Period three implies chaos, The American Mathematical Monthly, Vol. 82, No. 10. (Dec., 1975) 985{992 considered the historical origin of Chaos Theory if a continuous function f : I!I of an interval I ⊂ R has a periodic point of period 3, then it has periodic points of any order n 2 N there is also an uncountable subset of I of points that are not even \asymptotically periodic" this is a typical situation of chaotic dynamics chaos = sensitive dependence on the initial conditions (starting points that are very close have very different behavior under iterates of the function) Sharkovsky's Ordering and Chaos Introduction to Fractal Geometry and Chaos Matilde Marcolli Sharkovsky's theorem • in fact the result of Li and Yorke is a special case of a previous much more general theorem of Sharkovsky • Oleksandr M. -
Periodic Points and Entropies for Cellular Automata
Complex Systems 3 (1989) 117-128 Periodic Points and Entropies for Cellular Automata Rui M.A. Dillio CERN, SPS Division, CH-1211 Geneva, Switzerland and CFMC, Av. Prof Gama Pinto 2,1699 Lisbon Codex, Port ugal Abstract. For the class of permutive cellular automata the num ber of periodic points and the topological and metrical entropies are calculated. 1. Introduction Cellular automata (CA) are infinite sequences of symbols of a finite alphabet that evolve in time according to a definite local rule. We can take, for ex ample, a lattice where each vertex contains the value of a dynamical variable ranging over a finite set of numbers. At a certain t ime to the values on the vertices of the lattice take a definite value, but at time to + 1 , the values of the dynamical variable can change according to a law defined locally. This kind of system, as shown by von Neumann [8] can simulate a Turing ma chine, and specific examples exist where the cellular automaton is capable of uni versal computation [3]. The simplest examples of CA ru les are obtained when we restrict to one-dimensional lattices and the dynamic variable over each site of the lattice can take values on the finite field Z2 = {O,I} [10]. There is an extensive literature on the dynamics of one-dimensional CA and on the patterns generated by the evolution of the CA ru les in the ex tended phase space Z x Z+ [12]. These patterns appear to be organized in several complexity classes according to the behavior of the iterates of random initial conditions [11]. -
Topological Entropy of Quadratic Polynomials and Dimension of Sections of the Mandelbrot Set
TOPOLOGICAL ENTROPY OF QUADRATIC POLYNOMIALS AND DIMENSION OF SECTIONS OF THE MANDELBROT SET GIULIO TIOZZO Abstract. A fundamental theme in holomorphic dynamics is that the local geometry of parameter space (e.g. the Mandelbrot set) near a parameter re- flects the geometry of the Julia set, hence ultimately the dynamical properties, of the corresponding dynamical system. We establish a new instance of this phenomenon in terms of entropy. Indeed, we prove an \entropy formula" relating the entropy of a polynomial restricted to its Hubbard tree to the Hausdorff dimension of the set of rays landing on the corresponding vein in the Mandelbrot set. The results con- tribute to the recent program of W. Thurston of understanding the geometry of the Mandelbrot set via the core entropy. 1. Introduction Let us consider the family of quadratic polynomials 2 fc(z) := z + c; with c 2 C: The filled Julia set K(fc) of a quadratic polynomial fc is the set of points which do not escape to infinity under iteration, and the Julia set J(fc) is the boundary of K(fc). The Mandelbrot set M is the connectedness locus of the quadratic family, i.e. M := fc 2 C : the Julia set of fc is connectedg: A fundamental theme in the study of parameter spaces in holomorphic dynamics is that the local geometry of the Mandelbrot set near a parameter c reflects the geometry of the Julia set J(fc), hence it is related to dynamical properties of fc. In this paper we will establish a new instance of this principle, by comparing the topological entropy of quadratic polynomials to the Hausdorff dimension of certain sets of external rays.