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2013
The Schröder functional equation and its relation to
Journal of Physics A: Mathematical and Theoretical, 2008
The aim of this paper is to show that the invariant measure for a class of one dimensional chaotic maps, T (x), is an extended solution of the Schröder functional equation, q(T (x)) = λq(x), induced by them. Hence, we give an unified treatment of a collection of exactly solved examples worked out in the current literature. In particular, we show that these examples belongs to a class of functions introduced by Mira, (see text). Moreover, as a new example, we compute the invariant densities for a class of rational maps having the Weierstrass ℘ functions as an invariant one. Also, we study the relation between that equation and the well known Frobenius-Perron and Koopman's operators. PACS numbers: 05.45.-a 05.90.+m 02.30.Ks
Journal of Nonlinear Mathematical Physics, 2002
We give a hierarchy of many-parameter families of maps of the interval [0, 1] with an invariant measure and using the measure, we calculate Kolmogorov-Sinai entropy of these maps analytically. In contrary to the usual one-dimensional maps these maps do not possess period doubling or period-n-tupling cascade bifurcation to chaos, but they have single fixed point attractor at certain region of parameters space, where they bifurcate directly to chaos without having period-n-tupling scenario exactly at certain values of the parameters.
We generate new hierarchy of many-parameter family of maps of the interval [0, with an invariant measure, by composition of the chaotic maps of reference . Using the measure, we calculate Kolmogorov-Sinai entropy, or equivalently Lyapunov characteristic exponent, of these maps analytically, where the results thus obtained have been approved with numerical simulation. In contrary to the usual one-dimensional maps and similar to the maps of reference [1], these maps do not possess period doubling or period-n-tupling cascade bifurcation to chaos, but they have single fixed point attractor at certain region of parameters values, where they bifurcate directly to chaos without having period-n-tupling scenario exactly at these values of parameter whose Lyapunov characteristic exponent begins to be positive.
In this paper, we introduce chaotic measure for discrete and continuous dynamical systems and study some properties of measure chaotic systems. Also relationship between chaotic measure, ergodic and expansive measures is investigated. Finally, we prove a new version of variational principle for chaotic measure.
Physical Review E, 2002
We study local and global correlations between the naturally invariant measure of a chaotic one-dimensional map f and the conditionally invariant measure of the transiently chaotic map f H. The two maps differ only within a narrow interval H, while the two measures significantly differ within the images f l (H), where l is smaller than some critical number l c. We point out two different types of correlations. Typically, the critical number l c is small. The 2 value, which characterizes the global discrepancy between the two measures, typically obeys a power-law dependence on the width ⑀ of the interval H, with the exponent identical to the information dimension. If H is centered on an image of the critical point, then l c increases indefinitely with the decrease of ⑀, and the 2 value obeys a modulated power-law dependence on ⑀.
Chaos: An Interdisciplinary Journal of Nonlinear Science, 1993
One-dimensional maps with complete grammar are investigated in both permanent and transient chaotic cases. The discussion focuses on statistical characteristics such as Lyapunov exponent, generalized entropies and dimensions, free energies, and their finite size corrections. Our approach is based on the eigenvalue problem of generalized Frobenius-Perron operators, which are treated numerically as well as by perturbative and other analytical methods. The examples include the universal chaos function relevant near the period doubling threshold. Special emphasis is put on the entropies and their decay rates because of their invariance under the most general class of coordinate changes. Phase-transition-like phenomena at the border state of chaos due to intermittency and super instability are presented.
Communications in Mathematical Physics, 2003
We consider expansive homeomorphisms with the specification property. We give a new simple proof of a large deviation principle for Gibbs measures corresponding to a regular potential and we establish a general symmetry of the rate function for the large deviations of the antisymmetric part, under time-reversal, of the potential. This generalizes the Gallavotti-Cohen fluctuation theorem to a larger class of chaotic systems.
Nonlinear Analysis: Theory, Methods & Applications, 2000
Suppose that (X; ) is a topological dynamical system; that is X is a compact Hausdor space and : X → X is a homeomorphism. We can consider the linear operator T deÿned by T (f) = f • , where f is a function on X . If (X; ) and (Y; ) are topological dynamical systems, then they are isomorphic, and we write
Topology and its Applications, 2003
The infimum respectively minimum of the topological entropies in different spaces are studied for maps which are transitive or chaotic in the sense of Devaney (i.e., transitive with dense periodic points). After a short survey of results explicitly or implicitly known in the literature for zero and onedimensional spaces the paper deals with chaotic maps in some higher-dimensional spaces. The key role is played by the result saying that a chaotic map f in a compact metric space X without isolated points can always be extended to a triangular (skew product) map F in X × [0, 1] in such a way that F is also chaotic and has the same topological entropy as f . Moreover, the sets X × {0} and X × {1} are F -invariant which enables to use the factorization and obtain in such a way dynamical systems in the cone and in the suspension over X or in the space X × S 1 . This has several consequences. Among others, the best lower bounds for the topological entropy of chaotic maps on disks, tori and spheres of any dimensions are proved to be zero.
Pure and Applied Mathematics Journal, 2015
In this work, I studied a new class of topological λ-type chaos maps, λ-exact chaos and weakly λ-mixing chaos. Relationships with some other type of chaotic maps are given. I will list some relevant properties of λ-type chaotic map. The existence of chaotic behavior in deterministic systems has attracted researchers for many years. In engineering applications such as biological engineering, and chaos control, chaoticity of a topological system is an important subject for investigation. The definitions of λ-type chaos, λ-type exact chaos, λ-type mixing chaos, and weak λ-type mixing chaos are extended to topological spaces. This paper proves that these chaotic properties are all preserved under λr-conjugation. We have the following relationships: λ-type exact chaos⇒ λ-type mixing chaos ⇒ weak λ-type mixing chaos ⇒λ-type chaos.
Journal of Mathematical Physics, 2003
Hierarchy of one and many-parameter families of random trigonometric chaotic maps and one-parameter random elliptic chaotic maps of cn type with an invariant measure have been introduced. Using the invariant measure (Sinai-Ruelle-Bowen measure), the Kolmogrov-Sinai entropy of the random chaotic maps have been calculated analytically, where the numerical simulations support the results .
Pure and Applied Mathematics Journal, 2014
In this paper, we will study a new class of chaotic maps on locally compact Hausdorff spaces called Lambda-type chaotic maps and θ-type chaotic maps. The Lambda-type chaotic map implies chaotic map which implies θ-type chaotic map. Further, the definition of topological Lambda-type chaos implies John Tylar definition which implies topological θ-type chaos definition. Relationships with some other types of chaotic maps defined on topological spaces are given.
2011
We define new isomorphism-invariants for ergodic measure-preserving systems on standard probability spaces, called measure-theoretic chaos and measure-theoretic + chaos. These notions are analogs of the topological chaoses DC2 and its slightly stronger version (which we denote by DC1 1 2). We prove that: 1. If a topological system is measure-theoretically (measure-theoretically +) chaotic with respect to at least one of its ergodic measures then it is topologically DC2 (DC1 1 2) chaotic. 2. Every ergodic system with positive Kolmogorov-Sinai entropy is measure-theoretically + chaotic (even in a bit stronger uniform sense). We provide an example showing that the latter statement cannot be reversed, i.e., of a system of entropy zero with uniform measure-theoretic + chaos.
Ergodic Theory and Dynamical Systems, 2014
We define new isomorphism invariants for ergodic measure-preserving systems on standard probability spaces, called measure-theoretic chaos and measure-theoretic + chaos. These notions are analogs of the topological chaos DC2 and its slightly stronger version (which we denote by DC1 1 2 ). We prove that: (1) if a topological system is measuretheoretically (measure-theoretically + ) chaotic with respect to at least one of its ergodic measures then it is topologically DC2 (DC1 1 2 ) chaotic; (2) every ergodic system with positive Kolmogorov-Sinai entropy is measure-theoretically + chaotic (even in a slightly stronger uniform sense). We provide an example showing that the latter statement cannot be reversed, that is, of a system of entropy zero with uniform measure-theoretic + chaos.
Pramana, 2006
We introduce an interesting hierarchy of rational order chaotic maps that posses an invariant measure. In contrast to the previously introduced hierarchy of chaotic maps , with merely entropy production, the rational order chaotic maps can simultaneously produce and consume entropy . We compute the Kolmogorov-Sinai entropy of theses maps analytically and also their Lyapunov exponent numerically, where that obtained numerical results support the analytical calculations.
2002
The natural measure of a chaotic set in a phase-space region can be related to the dynamical properties of all unstable periodic orbits embedded in the chaotic set contained in that region. This result has been shown to be valid for hyperbolic chaotic invariant sets. The aim of this paper is to examine whether this result applies to nonhyperbolic, nonattracting chaotic saddles which lead to transient chaos in physical systems.
The aim of this paper is to establish some results in connection with the chaotic behaviours of the forward shift map on the generalised one-sided symbol space
Journal of Statistical Physics, 1984
We consider single-humped symmetric one-dimensional maps generating fully developed chaotic iterations specified by the property that on the attractor the mapping is everywhere two to one. To calculate the probability distribution function, and in turn the Lyapunov exponent and the correlation function, a perturbation expansion is developed for the invariant measure. Besides deriving some general results, we treat several examples in detail and compare our theoretical results with recent numerical ones. Furthermore, a necessary condition is deduced for the probability distribution function to be symmetric and an effective functional iteration method for the measure is introduced for numerical purposes.
2015
In this work, the definitions of alphatype chaos, alpha-type exact chaos, topologically alpha-type mixing chaos, and weak alpha -type mixing chaos are introduced and extended to topological spaces. This paper proves that these chaotic properties are all preserved under r conjugation. We have the following relationships: -type exact chaos⇒ -type mixing chaos ⇒ weak -type mixing chaos ⇒ -type chaos which implies chaos Keywords— alpha-type chaos, alpha-type exact chaos, topologically alpha-type mixing chaos, and weak alpha -type mixing chaos.
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