2021
DOI: 10.1007/s00023-021-01094-5
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Limit Theorems for Random Non-uniformly Expanding or Hyperbolic Maps with Exponential Tails

Abstract: We prove central limit theorems and related results for non-uniformly expanding random dynamical systems and general random Gibbs measures under some integrability conditions and some (relatively weak) mixing related assumptions on the random environment/base map. Some of our conditions also apply to maps which only expand on average, in an appropriate sense. This is the first set of conditions that allows to treat general non-uniformly expanding cases. A crucial step in our proofs can be viewed as effective m… Show more

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Cited by 13 publications
(37 citation statements)
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“…Let us also note that, in general, the random variable K(ω) comes from Oseledets theorem and it is not computable. In order to provide explicit conditions for quenched limit 132 Y. Hafouta theorems, in [28] several examples of non-uniformly expanding maps (which are stronger than expansion on average) were given with the property that…”
Section: 2mentioning
confidence: 99%
See 1 more Smart Citation
“…Let us also note that, in general, the random variable K(ω) comes from Oseledets theorem and it is not computable. In order to provide explicit conditions for quenched limit 132 Y. Hafouta theorems, in [28] several examples of non-uniformly expanding maps (which are stronger than expansion on average) were given with the property that…”
Section: 2mentioning
confidence: 99%
“…For instance, in [16,[20][21][22] almost sure invariance principle (ASIP, an almost sure approximation by a sum of independent Gaussians) was established for random expanding or hyperbolic maps T ω , in [19,31] Berry-Esseen theorems (optimal rates in the CLT) were obtained for similar classes of maps and in [17,18,23,31] local CLTs were achieved. In addition, in [27] several limit theorems were extended to random non-uniformly hyperbolic or expanding maps. We would also like to refer to [3] for related results concerning mixing rates for random non-uniformly hyperbolic maps and to [32] for related results concerning sequential dynamical systems, where an ASIP was obtained.…”
mentioning
confidence: 99%
“…Indeed, those are key tools to model many natural phenomena, including the transport in complex environments such as in the ocean or the atmosphere [3]: it is therefore crucial to understand their long term quantitative behavior. Among many remarkable contributions, we particularly emphasize those dealing with the decay of correlations [2,6,7,9,12,15], various (quenched or annealed) limit laws [1,4,16,17,18,19,20,30,31,32,39,43,44,48], as well as recent results devoted to the linear response of random dynamical systems [8,23,47]. For similar results in the closely related context of sequential dynamical systems, we refer to [10,11,33,35,36,37,29,42] and references therein.…”
Section: Introductionmentioning
confidence: 98%
“…Probably the first papers dealing with quenched limit theorems for random dynamical systems are [36,37], and since then limit theorems for several classes of random dynamical systems were vastly studied. We refer to [3,5,15,16,17,21,22,20,18,28,30,31,51,52] for a partial list of relatively recent results of this kind. We note that in many of the examples these results are obtained for the unique measure µ such that µ ω is absolutely continuous with respect to m. However, some results hold true even for maps T ω : E ω → E σω ⊂ X which are defined on random subsets of X (see [38]), where in this case the most notable choice of µ ω is the, so called, random Gibbs measure (see [28,43]).…”
mentioning
confidence: 99%
“…when T ω = T and ϕ(ω, x) = ϕ(x) do not depend on ω, many of the limit theorems follow from spectral properties of the transfer operator L T corresponding to T (namely, the dual of the Koopman operator g → g • T with respect to the underlying invariant measure µ), or from a sufficiently fast convergence of L n T towards a one dimensional projection. While several quenched limit theorems are based on an appropriate random counterpart of such spectral properties (see [15,16,17,21,22,20,18,28,30]), such annealed "spectral" techniques are not fully developed as the quenched ones. A very notable exception is the case of iid maps, discussed in the next section.…”
mentioning
confidence: 99%