Abstract
We address the analysis of the following problem: given a real Hölder potential f defined on the Bernoulli space and μ f its equilibrium state, it is known that this shift-invariant probability can be weakly approximated by probabilities in periodic orbits associated to certain zeta functions.
Given a Hölder function f > 0 and a value s such that 0 < s < 1, we can associate a shift-invariant probability ν s such that for each continuous function k we have
, where P(f) is the pressure of f, Fix n is the set of solutions of σ n(x) = x, for any n ∈ ℕ, and f n(x) = f(x) + f(σ (x)) + … + f(σ n−1(x)).
We call νs a zeta probability for f and s, because it can be obtained in a natural way from the dynamical zeta-functions. From the work of W. Parry and M. Pollicott it is known that ν s → µ f , when s → 1. We consider for each value c the potential c f and the corresponding equilibrium state μ cf . What happens with ν s when c goes to infinity and s goes to one? This question is related to the problem of how to approximate the maximizing probability for f by probabilities on periodic orbits. We study this question and also present here the deviation function I and Large Deviation Principle for this limit c → ∞, s → 1. We will make an assumption: for some fixed L we have limc→∞, s→1 c(1 − s) = L > 0. We do not assume here the maximizing probability for f is unique in order to get the L.D.P.
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Partially supported by CNPq, PRONEX — Sistemas Dinâmicos, INCT em Matemática, and beneficiary of CAPES financial support.
Supported by CNPq — Brazil — Ph.D. scholarship.
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Lopes, A.O., Mengue, J.K. Zeta measures and Thermodynamic Formalism for temperature zero. Bull Braz Math Soc, New Series 41, 449–480 (2010). https://doi.org/10.1007/s00574-010-0021-0
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DOI: https://doi.org/10.1007/s00574-010-0021-0