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Natural equilibrium states for multimodal maps., Preprint arXiv:0907.2406 (2009)

by G Iommi, M Todd
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Nice inducing schemes and the thermodynamics of rational maps

by Feliks Przytycki, Juan Rivera-letelier
"... Abstract. We consider the thermodynamic formalism of a complex rational map f of degree at least two, viewed as a dynamical system acting on the Riemann sphere. More precisely, for a real parameter t we study the (non-)existence of equilibrium states of f for the potential −tln |f ′ |, and the analy ..."
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Abstract. We consider the thermodynamic formalism of a complex rational map f of degree at least two, viewed as a dynamical system acting on the Riemann sphere. More precisely, for a real parameter t we study the (non-)existence of equilibrium states of f for the potential −tln |f ′ |, and the analytic dependence on t of the corresponding pressure function. We give a fairly complete description of the thermodynamic formalism of a rational map that is “expanding away from critical points ” and that has arbitrarily small “nice sets ” with some additional properties. Our results apply in particular to non-renormalizable polynomials without indifferent periodic points, infinitely renormalizable quadratic polynomials with a priori bounds, real quadratic polynomials, topological Collet-Eckmann rational maps, and to backward contracting rational maps. As an application, for these maps we describe the dimension spectrum of Lyapunov exponents, and of pointwise dimensions of the measure of
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...|f ′|dµ the Lyapunov exponent of µ. Given a real number t we define the pressure of f |J(f) for the potential −t ln |f ′| by, (1.1) P (t) := sup {hµ(f)− tχµ(f) | µ ∈ M (f)} . ∗Recently Iommi and Todd =-=[IT09]-=- have shown similar results for transitive multimodal maps with non-flat critical points as those presented here, but only obtaining that the pressure function is continuous differentiable, and withou...

EXTREME VALUE LAWS IN DYNAMICAL SYSTEMS FOR NON-SMOOTH OBSERVATIONS

by Ana Cristina Moreira Freitas, Jorge Milhazes Freitas, Mike Todd , 2010
"... We prove the equivalence between the existence of a non-trivial hitting time statistics law and Extreme Value Laws in the case of dynamical systems with measures which are not absolutely continuous with respect to Lebesgue. This is a counterpart to the result of the authors in the absolutely conti ..."
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We prove the equivalence between the existence of a non-trivial hitting time statistics law and Extreme Value Laws in the case of dynamical systems with measures which are not absolutely continuous with respect to Lebesgue. This is a counterpart to the result of the authors in the absolutely continuous case. Moreover, we prove an equivalent result for returns to dynamically defined cylinders. This allows us to show that we have Extreme Value Laws for various dynamical systems with equilibrium states with good mixing properties. In order to achieve these goals we tailor our observables to the form of the measure at hand.

A characterization of hyperbolic potentials of rational maps

by Irene Inoquio-renteria, Juan Rivera-letelier - Bull. Braz. Math. Soc. (N.S
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SYMBOLIC DYNAMICS FOR SURFACE DIFFEOMORPHISMS WITH POSITIVE ENTROPY

by Omri M. Sarig
"... 1.2. Symbolic dynamics 343 1.3. Markov partitions 344 ..."
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1.2. Symbolic dynamics 343 1.3. Markov partitions 344
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...ps (“towers”) which possess obvious infinite Markov partitions. Such extensions have been used in the study of one–dimensional systems with great success; see e.g. [Hof2], [Bu1], [Bru], [Ke2], [PSZ], =-=[IT]-=-, [Z]. For higher dimension, see [Bu4], [Bu2], [Bu5], [BT], [BY], [Y]. Unlike tower extensions, our coding is finite-to-one. This ensures that any ergodic invariant measure with high entropy can be li...

TRANSIENCE IN DYNAMICAL SYSTEMS

by Godofredo Iommi, Mike Todd
"... Abstract. We extend the theory of transience to general dynamical systems with no Markov structure assumed. This is linked to the theory of phase transitions. We also provide examples of new kinds of transient behaviour. 1. ..."
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Abstract. We extend the theory of transience to general dynamical systems with no Markov structure assumed. This is linked to the theory of phase transitions. We also provide examples of new kinds of transient behaviour. 1.
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... SYSTEMS 15 c) ...

The thermodynamic approach to multifractal analysis

by Vaughn Climenhaga - Ergod.Th. Dynam. Sys
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Geometric pressure for multimodal maps of the interval

by Feliks Przytycki, Juan Rivera-letelier
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...n K, and φ = −t log |f ′| (it is therefore clear that analyticity cannot hold at neither t = t− nor t = t+, as P (t) is affine to the left of t− and to the right of t+). Let us mention also the paper =-=[IT]-=- where, under the restriction that f has no preperiodic critical points, the existence of equilibria was proved for all −∞ = t− < t < t+. The authors proved that P (t) is of class C1 and that their me...

4 EQUILIBRIUM STATES, PRESSURE AND ESCAPE FOR MULTIMODAL MAPS WITH HOLES

by Mark Demers, Mike Todd
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...or ϕ1 if and only if µ is absolutely continuous with respect to Lebesgue measure. Moreover, it was shown in [BK] (unimodal Collet-Eckmann case, restricted t), [BT] (multimodal case, restricted t) and =-=[IT1]-=- (multimodal case, general t) that there is an equilibrium state µt corresponding to ϕt. The relation between these measures, the pressure and the Lyapunov spectrum was shown in [IT2]. The classical B...

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by Katrin Gelfert, Feliks Przytycki, Micha, L Rams
"... Abstract. We study the dimension spectrum of Lyapunov exponents for multimodal maps of the interval and their generalizations. We also ..."
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Abstract. We study the dimension spectrum of Lyapunov exponents for multimodal maps of the interval and their generalizations. We also

EXTREME VALUE LAWS IN DYNAMICAL SYSTEMS FOR

by Ana Cristina, Moreira Freitas, Jorge Milhazes Freitas, Mike Todd
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...f this, much more is known for HTS to balls in one dimension. For example if f : I → I is a multimodal map of the unit interval I and φ = −t log |Df | is a potential with an equilibrium state µt (see =-=[IT09]-=- for the most general result in on existence of such equilibrium states), it was proved in [BT09a] that the system has exponential HTS EXTREME VALUE LAWS IN DYNAMICAL SYSTEMS FOR NON-SMOOTH OBSERVATIO...

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