Boundary Values of the Thurston Pullback Map

Total Page:16

File Type:pdf, Size:1020Kb

Boundary Values of the Thurston Pullback Map Boundary Values of the Thurston Pullback Map Russell Lodge Indiana University Bloomington, Indiana [email protected] July 3, 2012 Abstract The Thurston characterization and rigidity theorem gives a beauti- ful description of when a postcritically finite topological branched cover mapping the 2-sphere to itself is Thurston equivalent to a rational func- tion. Thurston equivalence remains mysterious, but great strides were taken when Bartholdi and Nekrashevych used iterated monodromy groups to solve the \Twisted Rabbit Problem" which sought to identify the Thurston class of the rabbit polynomial composed with an arbi- trary Dehn twist. Selinger showed that the Thurston pullback map on Teichm¨ullerspace can be extended to the Weil-Petersson boundary. We compute these boundary values for the pullback map associated to 3z2 f(z) = 2z3+1 and demonstrate how the dynamical properties of this map on the boundary can be used as an invariant to solve the twisting problem for f. Contents 1 Introduction 2 1.1 Thurston's Theorem . 4 1.2 Boundary Values of the Pullback Map . 5 1.3 The Twisting Problem . 6 1.4 Outline . 7 2 Thurston Maps with n Postcritical Points 8 2.1 Notation, Definitions, and Examples . 8 2.2 Two definitions of Teichm¨ullerspace; Virtual Endomorphisms 12 2.3 Schreier Graphs and the Reidemeister-Schreier Algorithm . 22 2.4 Iterated Monodromy Groups and Wreath Recursions . 23 1 3 General facts in the case jPf j = 4 29 3z2 4 Analysis of a specific example: f(z) = 2z3+1 37 4.1 The Dynamical Plane of f .................... 37 4.2 The Correspondence on Moduli Space . 41 4.3 The Virtual Endomorphism and Wreath Recursion on Moduli Space . 43 4.4 The Wreath Recursion on the Dynamical Plane; Covering and Hurwitz Equivalence . 49 5 Boundary Values of σf 52 5.1 The Boundary Maps to the Boundary . 52 5.2 Dynamical behavior of φf .................... 53 6 Properties of σf : Q ! Q 61 7 Slopes of Curves in Cb n P when jP j = 4 66 7.1 Slopes in Cb n P when jP j =4 .................. 66 7.2 Slopes in Cb n P when P = f0; 1; !; !¯g . 69 8 The Twisting Problem for f 71 8.1 Limiting behavior of the Extended Virtual Endomorphism . 71 8.2 Solution to the Twisting Problem . 78 9 Future Work 83 1 Introduction Broadly speaking, this dissertation deals with the interplay between geome- try, topology, algebra and complex dynamics; the primary focus of this work is Teichm¨ullerspace and Thurston's characterization theorem for rational maps. In the early 1980's, John Hubbard and Adrien Douady highlighted a close relationship between combinatorics and complex dynamics when they created combinatorial models for the Julia sets of critically finite polyno- mials using Hubbard trees [7]. Critically finite quadratic polynomials are highly significant because they could be used to prove the famous conjec- ture that hyperbolicity is dense|this conjecture was shown by McMullen to be equivalent to the statement that certain quadratics can be approxi- mated by a sequence of critically finite quadratics obtained by a procedure 2 called renormalization [20]. Douady and Hubbard also present an algorithm that in principle finds the formula for a polynomial realizing any admissible Hubbard tree. These results are very illuminating, and there are a number of other combinatorial invariants that can faithfully encode polynomials, al- lowing much to be said about the relationship between combinatorics and Julia sets in the case of polynomials. Complex rational functions are another matter, however, and it is not known how to extend results for polynomials to the rational case. This sets the stage for Thurston's theorem. Complex rational func- tions are a very rigid class of functions (e.g. they are conformal outside of a finite set), and finding explicit formulas for one that realizes partic- ular combinatorial data can be challenging. Thus, we focus our attention on a more flexible class of functions. A Thurston map is a critically fi- nite orientation-preserving branched cover from the two-sphere to itself. To pursue the agenda of relating combinatorics to dynamics, one can create a combinatorial model of a dynamical system using Thurston maps, and then Thurston's theorem characterizes when the Thurston map is equivalent to a rational function. Furthermore, the theorem asserts a rigidity result|if the Thurston map is equivalent to a rational function, this rational function is es- sentially unique (ignoring a family of well-understood Euclidean examples). Thurston's theorem for rational functions is proven in [12] using iteration of an analytic map on Teichm¨ullerspace called Thurston's pullback map. The proof parallels the proof of Thurston's theorem on the hyperbolization of 3-manifolds, which studies dynamics of the skinning map on Teichm¨uller space. Thurston's pullback map is very mysterious, and one goal of my research has been to understand its dynamics on the Weil-Petersson completion of Teichm¨ullerspace using the fact of Selinger that the pullback map extends to the boundary [30]. I did this for the Thurston pullback map associated to 3z2 the rational function f(z) = 2z3+1 because f was investigated in [8]. This paper showed that the Thurston pullback map associated to f is surjective, and up to some nondynamical equivalence it is essentially the only pullback function where this property has been observed. A second major focus of my work has been to better understand the notion of equivalence used in Thurston's theorem. Pilgrim described the lack of solution to the Twisted Rabbit Problem a "humbling reminder" of the lack of suitable invariants for Thurston equivalence [27], and though the problem has been solved, the need for invariants remains. The following study of the Thurston pullback map and Thurston equivalence exploit some rich connections between the 3 Thurston pullback map, combinatorics, Weil-Petersson geometry, hyperbolic geometry, group theory, and arithmetic dynamics. 1.1 Thurston's Theorem Let F be an orientation-preserving branched cover which maps the two- sphere to itself by degree greater than one. Denote by PF the postcritical set as defined in Section 2.1. If PF is finite, F is called a Thurston map. There are several valuable sources for producing examples of Thurston maps: an obvious example would be any post-critically finite rational maps with degree greater than two. Finite subdivision rules of the two-sphere are a con- venient way to produce combinatorial models of Thurston maps, and they have been studied extensively in the recent past [9]. A third way to produce examples of Thurston maps is by mating two critically finite polynomials of the same degree [23]. Having shown that a wealth of examples of Thurston maps exist, we define Thurston equivalence and then state Thurston's the- orem: Definition: Let F and G be Thurston maps with postcritical sets PF and PG respectively. Then F is Thurston equivalent to G if there are orien- 2 2 tation preserving homeomorphisms h0; h1 :(S ;PF ) −! (S ;PG) with h0 homotopic to h1 rel PF , so that the following commutes: 2 h1 2 (S ;PF ) / (S ;PG) F G 2 h0 2 (S ;PF ) / (S ;PG) Thurston's Theorem: Let F be a Thurston map which is not a Latt`es example. Then F is Thurston equivalent to a rational map if and only if the Thurston pullback map has a fixed point. Furthermore, if F is equivalent to a rational map, this rational map is unique up to M¨obiusconjugation. Thurston maps are called obstructed if they are not equivalent to a ra- tional function. A different formulation of Thurston's theorem from the one above gives a better sense for why certain Thurston maps are or are not obstructed; having a fixed point of the pullback map is equivalent to the Thurston map not having a special family of simple closed curves in the two- sphere that behave a certain way under preimage. The mapping properties of curves under preimage of a Thurston map have deep implications for the pullback map on Teichm¨ullerspace, and we will pursue this theme in both 4 of the following sections. It is also worth noting that mapping properties of simple closed curves play an important role in the three other groundbreak- ing theorems proved by Thurston relating geometry and topology, as noted by John Hubbard [15]. Recently there has also been interest in non-dynamical problems involv- ing branched covers of the sphere by higher genus surfaces. See for example the discussion of the Birman-Hilden property in [5, 13]. As was the case in the dynamical setting just described, the preimages of essential curves seem to be significant actors. 1.2 Boundary Values of the Pullback Map Thurston's pullback map is very complicated|it is transcendental, and in all known examples it is infinite-to-one. It may be surprising, then, that 3z2 the pullback map associated to f(z) = 2z3+1 has boundary values that can be computed by transforming the even continued fraction expansions of rational numbers by a prescribed algorithm (see [8] for an image of the Thurston pullback map studied here). We call a simple closed curve γ ⊂ Cb n PF essential if both components bounded by γ contain at least two post-critical points. The collection of homotopy classes of essential curves in Cb n PF can be put in correspondence with the rational numbers when there are four post-critical points. Further- more, when jPF j = 4, it is a standard fact that Teichm¨ullerspace can be identified with the upper half-plane in such a way that the Weil-Petersson p completion is obtained by adding the rational points q + 0i along with the 1 point 0 to the boundary of the upper half-plane where each point corre- sponds to collapsing the sphere with four marked points along the curve p corresponding to q .
Recommended publications
  • STRONG REGULARITY 3 Ergodic Theorem Produces Lyapunov Exponents (W.R.T
    STRONG REGULARITY by Pierre Berger and Jean-Christophe Yoccoz 1. Uniformly hyperbolic dynamical systems The theory of uniformly hyperbolic dynamical systems was constructed in the 1960’s under the dual leadership of Smale in the USA and Anosov and Sinai in the Soviet Union. It is nowadays almost complete. It encompasses various examples [Sma67]: expanding maps, horseshoes, solenoid maps, Plykin attractors, Anosov maps and DA, all of which are basic pieces. We recall standard definitions. Let f be a C1-diffeomorphism f of a finite dimen- sional manifold M. A compact f-invariant subset Λ ⊂ M is uniformly hyperbolic if the restriction to Λ of the tangent bundle TM splits into two continuous invariant subbundles TM|Λ= Es ⊕ Eu, Es being uniformly contracted and Eu being uniformly expanded. Then for every z ∈ Λ, the sets W s(z)= {z′ ∈ M : lim d(f n(z),f n(z′))=0}, n→+∞ W u(z)= {z′ ∈ M : lim d(f n(z),f n(z′))=0} n→−∞ are called the stable and unstable manifolds of z. They are immersed manifolds tangent at z to respectively Es(z) and Eu(z). s arXiv:1901.09430v1 [math.DS] 27 Jan 2019 The ǫ-local stable manifold Wǫ (z) of z is the connected component of z in the intersection of W s(z) with a ǫ-neighborhood of z. The ǫ-local unstable manifold u Wǫ (z) is defined likewise. Definition 1.1. — A basic set is a compact, f-invariant, uniformly hyperbolic set Λ which is transitive and locally maximal: there exists a neighborhood N of Λ such that n Λ= ∩n∈Zf (N).
    [Show full text]
  • DOUBLE STANDARD MAPS 1. Introduction It Is a Usual
    DOUBLE STANDARD MAPS MICHALMISIUREWICZ AND ANA RODRIGUES Abstract. We investigate the family of double standard maps of the circle onto itself, given by fa,b(x) = 2x + a + (b/π) sin(2πx) (mod 1), where the parameters a, b are real and 0 ≤ b ≤ 1. Similarly to the well known family of (Arnold) standard maps of the circle, Aa,b(x) = x + a + (b/(2π)) sin(2πx) (mod 1), any such map has at most one attracting periodic orbit and the set of parameters (a, b) for which such orbit exists is divided into tongues. However, unlike the classical Arnold tongues, that begin at the level b = 0, for double standard maps the tongues begin at higher levels, depending on the tongue. Moreover, the order of the tongues is different. For the standard maps it is governed by the continued fraction expansions of rational numbers; for the double standard maps it is governed by their binary expansions. We investigate closer two families of tongues with different behavior. 1. Introduction It is a usual procedure that in order to understand the behavior of a system in higher dimension one investigates first a one-dimensional system that is somewhat similar. The classical example is the H´enonmap and similar systems, where a serious progress occurred only after unimodal interval maps have been thoroughly understood. Another example of this type was investigation by V. Arnold of the family of standard maps of the circle, given by the formula b (1.1) A (x) = x + a + sin(2πx) (mod 1) a,b 2π (when we write “mod 1,” we mean that both the arguments and the values are taken modulo 1).
    [Show full text]
  • An Entire Transcendental Family with a Persistent Siegel Disk
    An entire transcendental family with a persistent Siegel disk Rub´en Berenguel, N´uria Fagella March 12, 2009 Abstract We study the class of entire transcendental maps of finite order with one critical point and one asymptotic value, which has exactly one finite pre-image, and having a persistent Siegel disk. After normalization ∗ this is a one parameter family fa with a ∈ C which includes the semi- standard map λzez at a = 1, approaches the exponential map when a → 0 and a quadratic polynomial when a → ∞. We investigate the stable components of the parameter plane (capture components and semi-hyperbolic components) and also some topological properties of the Siegel disk in terms of the parameter. 1 Introduction Given a holomorphic endomorphism f : S → S on a Riemann surface S we consider the dynamical system generated by the iterates of f, denoted by n) n f = f◦ ··· ◦f. The orbit of an initial condition z0 ∈ S is the sequence + n O (z0)= {f (z0)}n N and we are interested in classifying the initial condi- ∈ tions in the phase space or dynamical plane S, according to the asymptotic behaviour of their orbits when n tends to infinity. There is a dynamically natural partition of the phase space S into the Fatou set F (f) (open) where the iterates of f form a normal family and the Julia set J (f)= S\F (f) which is its complement (closed). If S = C = C ∪∞ then f is a rational map. If S = C and f does not extend to the point at infinity, then f is an entire transcendental map, b that is, infinity is an essential singularity.
    [Show full text]
  • Elliptic Bubbles in Moser's 4D Quadratic Map: the Quadfurcation
    Elliptic Bubbles in Moser's 4DQuadratic Map: the Quadfurcation ∗ Arnd B¨ackery and James D. Meissz Abstract. Moser derived a normal form for the family of four-dimensional, quadratic, symplectic maps in 1994. This six-parameter family generalizes H´enon'subiquitous 2d map and provides a local approximation for the dynamics of more general 4D maps. We show that the bounded dynamics of Moser's family is organized by a codimension-three bifurcation that creates four fixed points|a bifurcation analogous to a doubled, saddle-center|which we call a quadfurcation. In some sectors of parameter space a quadfurcation creates four fixed points from none, and in others it is the collision of a pair of fixed points that re-emerge as two or possibly four. In the simplest case the dynamics is similar to the cross product of a pair of H´enonmaps, but more typically the stability of the created fixed points does not have this simple form. Up to two of the fixed points can be doubly-elliptic and be surrounded by bubbles of invariant two-tori; these dominate the set of bounded orbits. The quadfurcation can also create one or two complex-unstable (Krein) fixed points. Special cases of the quadfurcation correspond to a pair of weakly coupled H´enonmaps near their saddle-center bifurcations. Key words. H´enonmap, symplectic maps, saddle-center bifurcation, Krein bifurcation, invariant tori AMS subject classifications. 37J10 37J20 37J25 70K43 1. Introduction. Multi-dimensional Hamiltonian systems model dynamics on scales rang- ing from zettameters, for the dynamics of stars in galaxies [1, 2], to nanometers, in atoms and molecules [3, 4].
    [Show full text]
  • A Partial Justification of Greene's Criterion For
    A PARTIAL JUSTIFICATION OF GREENE'S CRITERION FOR CONFORMALLY SYMPLECTIC SYSTEMS RENATO C. CALLEJA, ALESSANDRA CELLETTI, CORRADO FALCOLINI, AND RAFAEL DE LA LLAVE Abstract. Greene's criterion for twist mappings asserts the existence of smooth in- variant circles with preassigned rotation number if and only if the periodic trajectories with frequency approaching that of the quasi-periodic orbit are linearly stable. We formulate an extension of this criterion for conformally symplectic systems in any dimension and prove one direction of the implication, namely that if there is a smooth invariant attractor, we can predict the eigenvalues of the periodic orbits whose frequencies approximate that of the tori. The proof of this result is very different from the proof in the area preserving case, since in the conformally symplectic case the existence of periodic orbits requires adjusting parameters. Also, as shown in [13], in the conformally symplectic case there are no Birkhoff invariants giving obstructions to linearization near an invariant torus. As a byproduct of the techniques developed here, we obtain quantitative information on the existence of periodic orbits in the neighborhood of quasi-periodic tori and we provide upper and lower bounds on the width of the Arnold tongues in n-degrees of freedom conformally symplectic systems. Contents 1. Introduction 2 1.1. The Greene's criterion 2 1.2. Greene's criterion for conformally symplectic systems 3 1.3. Organization of the paper 6 2. Local behavior near rotational Lagrangian tori in conformally symplectic systems 6 2.1. Conformally symplectic systems 6 2.2. Local behavior in a neighborhood of a KAM torus 7 3.
    [Show full text]
  • Bifurcations, Mode Locking, and Chaos in a Dissipative System
    The Bogdanov Map: Bifurcations, Mode Locking, and Chaos in a Dissipative System David K. Arrowsmith, School of Mathematical Sciences Queen Mary and Westfield College University of London Mile End Road London E1 4NS, UK Julyan H. E. Cartwright, Departament de F´ısica Universitat de les Illes Balears 07071 Palma de Mallorca, Spain Alexis N. Lansbury, Department of Physics Brunel, The University of West London Uxbridge, Middlesex UB8 3PH, UK &ColinM.Place.∗ Int. J. Bifurcation and Chaos, 3,803–842,1993 We investigate the bifurcations and basins of attraction in the Bog- danov map, a planar quadratic map which is conjugate to the Henon´ area-preserving map in its conservative limit. It undergoesaHopf bifurcation as dissipation is added, and exhibits the panoply of mode locking, Arnold tongues, and chaos as an invariant circle grows out, finally to be destroyed in the homoclinic tangency of the manifolds of aremotesaddlepoint.TheBogdanovmapistheEulermapofatwo- dimensional system of ordinary differential equations firstconsidered by Bogdanov and Arnold in their study of the versal unfolding of the double-zero-eigenvalue singularity, and equivalently of avectorfield invariant under rotation of the plane by an angle 2π.Itisauseful system in which to observe the effect of dissipative perturbations on Hamiltonian structure. In addition, we argue that the Bogdanov map provides a good approximation to the dynamics of the Poincaremaps´ of periodically forced oscillators. ∗Formerly: Department of Mathematics, Westfield College, University of London, UK. 1 1. Introduction Tisnowwellknownthatthestudyofsystemsofordinarydifferential equations, which commonly arise in dynamical systems investigated in I many fields of science, can be aided by utilizing the surface-of-section technique of Poincaremaps.The´ Poincar´e or return map of a system of or- dinary differential equations reduces the dimension of the problem, replac- ing an n-dimensional set of ordinary differential equations with an (n 1)- dimensional set of difference equations.
    [Show full text]
  • NL3238 the Standard Map 1 NL3238 the Standard Map
    NL3238 The Standard Map 1 NL3238 The Standard Map Derivation The standard or Taylor-Chirikov map is a family of area-preserving maps, z0 = f(z) with z = (x, y), given by k x0 = x + y − sin(2πx) 2π k y0 = y − sin(2πx) . (1) 2π Here x is a periodic configuration variable, and is usually computed “mod 1,” and y ∈ R is the momentum variable. The map has a single parameter k which represents the strength of the nonlinear kick. This map was first proposed by Bryan Taylor and then independently obtained by Boris Chirikov to describe the dynamics of magnetic field lines. The standard map and H´enon’sarea-preserving quadratic map provide extensively studied paradigms for chaotic Hamiltonian dynamics. The standard map is an exact symplectic map of the cylinder. Since x0(x, y) is a monotone function of y for each x, it is also an example of a monotone twist map (see Aubry–Mather theory). Every twist map has a Lagrangian generating function; the 0 1 0 2 k standard map is generated by F (x, x ) = 2 (x − x) + 4π2 cos(2πx), so that y = −∂F/∂x and y0 = ∂F/∂x0. The map can also be obtained from a discrete Lagrangian variational principle: define the discrete action for any configuration sequence . , xt−1, xt, xt+1,... as the formal sum X A[. , xt−1, xt, xt+1,...] = F (xt, xt+1) . (2) t Then an orbit is a sequence which is a critical point of A; this gives the discrete Euler- Lagrange equation k x − 2x + x = − sin(2πx ) .
    [Show full text]
  • Pseudo-Random Number Generator Based on Logistic Chaotic System
    entropy Article Pseudo-Random Number Generator Based on Logistic Chaotic System Luyao Wang and Hai Cheng * Electronic Engineering College, Heilongjiang University, Harbin 150080, China; [email protected] * Correspondence: [email protected] Received: 23 August 2019; Accepted: 27 September 2019; Published: 30 September 2019 Abstract: In recent years, a chaotic system is considered as an important pseudo-random source to pseudo-random number generators (PRNGs). This paper proposes a PRNG based on a modified logistic chaotic system. This chaotic system with fixed system parameters is convergent and its chaotic behavior is analyzed and proved. In order to improve the complexity and randomness of modified PRNGs, the chaotic system parameter denoted by floating point numbers generated by the chaotic system is confused and rearranged to increase its key space and reduce the possibility of an exhaustive attack. It is hard to speculate on the pseudo-random number by chaotic behavior because there is no statistical characteristics and infer the pseudo-random number generated by chaotic behavior. The system parameters of the next chaotic system are related to the chaotic values generated by the previous ones, which makes the PRNG generate enough results. By confusing and rearranging the output sequence, the system parameters of the previous time cannot be gotten from the next time which ensures the security. The analysis shows that the pseudo-random sequence generated by this method has perfect randomness, cryptographic properties and can pass the statistical tests. Keywords: logistic chaotic system; PRNG; Pseudo-random number sequence 1. Introduction With the rapid development of communication technology and the wide use of the Internet and mobile networks, people pay more and more attention to information security.
    [Show full text]
  • On Stochastic Sea of the Standard Map
    ON STOCHASTIC SEA OF THE STANDARD MAP ANTON GORODETSKI Abstract. Consider a generic one-parameter unfolding of a homoclinic tangency of an area pre- serving surface diffeomorphism. We show that for many parameters (residual subset in an open set approaching the critical value) the corresponding diffeomorphism has a transitive invariant set Ω of full Hausdorff dimension. The set Ω is a topological limit of hyperbolic sets and is accumulated by elliptic islands. As an application we prove that stochastic sea of the standard map has full Hausdorff dimension for sufficiently large topologically generic parameters. Keywords: standard map, conservative dynamics, hyperbolic set, Newhouse phenomena, persistent tangencies, Hausdorff dimension, homoclinic picture, homoclinic class, stochastic layer. MSC 2000: 37E30, 37D45, 37J45, 37J20. 1. Introduction and Main Results Here we prove that stochastic sea of the Taylor-Chirikov standard map (i.e. the set of orbits with non-zero Lyapunov exponents) has full Hausdorff dimension for large topologically generic parameters. In order to do so we show that a perturbation of an area preserving diffeomorphism with a homoclinic tangency has hyperbolic invariant sets of almost full Hausdorff dimension. 1.1. Standard map. The simplest and most famous symplectic system with highly non-trivial dy- namics is the Taylor-Chirikov standard map of the two{dimensional torus T2, given by 2 (1) fk(x; y) = (x + y + k sin(2πx); y + k sin(2πx)) mod Z : This family is related to numerous physical problems, see for example [C], [I], [SS]. For k = 0 the map f0(x; y) = (x+y; y) is completely integrable, and leaves the circles y = const invariant.
    [Show full text]
  • Research Article a Novel Pseudorandom Bit Generator Based on Chirikov Standard Map Filtered with Shrinking Rule
    Hindawi Publishing Corporation Mathematical Problems in Engineering Volume 2014, Article ID 986174, 4 pages http://dx.doi.org/10.1155/2014/986174 Research Article A Novel Pseudorandom Bit Generator Based on Chirikov Standard Map Filtered with Shrinking Rule Borislav Stoyanov and Krasimir Kordov Faculty of Mathematics and Informatics, Konstantin Preslavski University of Shumen, 9712 Shumen, Bulgaria Correspondence should be addressed to Borislav Stoyanov; [email protected] Received 12 February 2014; Accepted 3 June 2014; Published 30 June 2014 Academic Editor: Jonathan N. Blakely Copyright © 2014 B. Stoyanov and K. Kordov. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. This communication proposes a simplified model of pseudorandom bit generator, based on two Chirikov standard maps filtered with shrinking rule. The study also demonstrates that the tedgenera keystreams have excellent properties of randomness and resistance to statistical attacks, which is proven by using the NIST, ENT, and DIEHARD testing suites. 1. Introduction 2. The Proposed Pseudorandom Bit Generator The chaotic maps and the shrinking rules have been used The Chirikov standard map is an area-conserving chaotic widely in the fields of random simulations and secure map defined by a set of difference equations: communications. Patidar and Sud [1] introduced a pseudo- +1 = +sin (), random bit generator with good cryptographic properties by using two Chirikov standard maps [2]combinedwitha +1 =+1 +, threshold function. Lian et al. [3]andFuetal.[4]proposed (1) standard map-based pseudorandom confusion processes, where the quantities and (momentum and coordinate) which they used in chaotic image encryption schemes.
    [Show full text]
  • Three-Dimensional Hénon-Like Maps and Wild Lorenz-Like
    February 4, 2006 13:56 01418 International Journal of Bifurcation and Chaos, Vol. 15, No. 11 (2005) 3493–3508 c World Scientific Publishing Company THREE-DIMENSIONAL HENON-LIKE´ MAPS AND WILD LORENZ-LIKE ATTRACTORS S. V. GONCHENKO Inst. Appl. Math. and Cyb., Nizhny Novgorod State Univ., 10 Ulyanova st., Nizhny Novgorod, 603005, Russia [email protected] I. I. OVSYANNIKOV Radio and Physical Dept., Nizhny Novgorod State Univ., 23 Gagarina av., Nizhny Novgorod, 603000, Russia [email protected] C. SIMO´ Departament Matem`atica Aplicada i An`alisi, Universitat de Barcelona, Gran Via, 585, 08007 Barcelona, Spain [email protected] D. TURAEV Department of Math., Ben Gurion University, Beer Sheva 84105, Israel [email protected] Received October 15, 2004; Revised February 15, 2005 We discuss a rather new phenomenon in chaotic dynamics connected with the fact that some three-dimensional diffeomorphisms can possess wild Lorenz-type strange attractors. These attractors persist for open domains in the parameter space. In particular, we report on the by SWETSWISE on 11/14/12. For personal use only. existence of such domains for a three-dimensional H´enon map (a simple quadratic map with a constant Jacobian which occurs in a natural way in unfoldings of several types of homo- clinic bifurcations). Among other observations, we have evidence that there are different types of Lorenz-like attractor domains in the parameter space of the 3D H´enon map. In all cases the maximal Lyapunov exponent, Λ1, is positive. Concerning the next Lyapunov exponent, Λ2, Int. J. Bifurcation Chaos 2005.15:3493-3508.
    [Show full text]
  • The Standard
    STANDARD MAP The standard map also describes the relativistic The standard or Taylor–Chirikov map is a family of cyclotron, and is the equilibrium condition for a area-preserving maps, z = f(z)where z = (x, y) is the chain of masses connected by harmonic springs in original position and z = (x,y) the new position after a periodic potential—the Frenkel–Kontorova model application of the map, which is defined by introduced in 1938 (Meiss, 1992). Similar maps include Chirikov’s separatrix map (valid near the separatrix of k a resonance), the Kepler map (describing the motion x = x + y − ( πx), sin 2 of comets under the influence of Jupiter as well as 2π (1) k a classical hydrogen atom in a microwave field), y = y − sin(2πx). 2π and the Fermi map (for a ball bouncing between oscillating walls) (Lichtenberg & Lieberman, 1992). Here x is a periodic configuration variable (usually The higher-dimensional version is the Froeshlé map computed modulo 1), y ∈ R is the momentum variable, (See Symplectic maps). and the parameter k represents the strength of a nonlinear kick. This map was first proposed in 1968 by Symmetries Bryan Taylor and then independently obtained by Boris Chirikov to describe the dynamics of magnetic field The standard map f has a number of symmetries that lines. The standard map and Hénon’s area-preserving lead to special dynamical behavior. To see these, it is quadratic map are extensively studied paradigms for convenient to lift the map from the cylinder to the plane chaotic Hamiltonian dynamics. by extending the angle variable x to R.
    [Show full text]