2018
DOI: 10.48550/arxiv.1811.07775
|View full text |Cite
Preprint
|
Sign up to set email alerts
|

Sharp polynomial bounds on decay of correlations for multidimensional nonuniformly hyperbolic systems and billiards

Abstract: Gouëzel and Sarig introduced operator renewal theory as a method to prove sharp results on polynomial decay of correlations for certain classes of nonuniformly expanding maps. In this paper, we apply the method to planar dispersing billiards and multidimensional nonMarkovian intermittent maps.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

2020
2020
2021
2021

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(6 citation statements)
references
References 50 publications
0
6
0
Order By: Relevance
“…Under similar conditions to the Definition 2.9, [VZ16] proved that µ U (R > n) characterizes the optimal bound for the decay rates of correlations for sufficiently good observables supported on U (see the Theorem 1.3 in [VZ16]); [BMT18] uses operator renewal theory as a method to prove also sharp results on polynomial decay of correlations (see Theorem 3.1 in [BMT18]). For many purposes the aperiodicity in the Definition 2.5 is irrelevant provided the dynamic f : (M, µ) → (M, µ) is mixing (see the Remark 2.2 in [BMT18]). Indeed all dynamical systems, which we consider in applications (section 6), do have a Markov partition.…”
Section: For Almost Every Pointmentioning
confidence: 92%
“…Under similar conditions to the Definition 2.9, [VZ16] proved that µ U (R > n) characterizes the optimal bound for the decay rates of correlations for sufficiently good observables supported on U (see the Theorem 1.3 in [VZ16]); [BMT18] uses operator renewal theory as a method to prove also sharp results on polynomial decay of correlations (see Theorem 3.1 in [BMT18]). For many purposes the aperiodicity in the Definition 2.5 is irrelevant provided the dynamic f : (M, µ) → (M, µ) is mixing (see the Remark 2.2 in [BMT18]). Indeed all dynamical systems, which we consider in applications (section 6), do have a Markov partition.…”
Section: For Almost Every Pointmentioning
confidence: 92%
“…To obtain upper and lower bounds on mixing rates we further induce T 1 (the first return map of T to Y ) to a two-sided Young tower. This will allows us to apply [3,Theorem 7.4].…”
Section: Mixing Ratesmentioning
confidence: 99%
“…The article [3] requires one more condition. We need to check that there exist C > 0 and θ ∈ (0, 1) such that for every z, z ∈ Q and n ≥ 1, d(T 2 n z, T 2 n z ) ≤ C(θ n + θ s(z,z )−n ).…”
Section: Mixing Ratesmentioning
confidence: 99%
See 2 more Smart Citations