2004
DOI: 10.4007/annals.2004.159.1275
|View full text |Cite
|
Sign up to set email alerts
|

On contact Anosov flows

Abstract: Exponential decay of correlations for C 4 contact Anosov flows is established. This implies, in particular, exponential decay of correlations for all smooth geodesic flows in strictly negative curvature.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4

Citation Types

1
268
0

Year Published

2009
2009
2023
2023

Publication Types

Select...
4
2

Relationship

1
5

Authors

Journals

citations
Cited by 211 publications
(269 citation statements)
references
References 38 publications
1
268
0
Order By: Relevance
“…Just like in [30], we do not claim that the transfer operator L 1 associated to the time-one map T 1 has a spectral gap. However, the resolvent method we adapt from [30] gives us a precise description of the spectrum of the generator X of the semigroup of operators L t in a half-plane large enough to deduce exponential decay of correlations (see Corollaries 3.6 and 3.10). The spaces H r,s,q p that we shall use are a modification (see Subsection 2.2) of the spaces H r,s p (s < 0 < r and 1 < p < ∞) of [6] for piecewise hyperbolic maps (the spaces in [6] generalise earlier constructions in [5] and [3], more directly related to standard Triebel spaces).…”
Section: Contentsmentioning
confidence: 99%
See 4 more Smart Citations
“…Just like in [30], we do not claim that the transfer operator L 1 associated to the time-one map T 1 has a spectral gap. However, the resolvent method we adapt from [30] gives us a precise description of the spectrum of the generator X of the semigroup of operators L t in a half-plane large enough to deduce exponential decay of correlations (see Corollaries 3.6 and 3.10). The spaces H r,s,q p that we shall use are a modification (see Subsection 2.2) of the spaces H r,s p (s < 0 < r and 1 < p < ∞) of [6] for piecewise hyperbolic maps (the spaces in [6] generalise earlier constructions in [5] and [3], more directly related to standard Triebel spaces).…”
Section: Contentsmentioning
confidence: 99%
“…It follows that the "bounded" term in our Lasota-Yorke bound (Lemma 3.1) is not really bounded. The "compact" term in the Lasota-Yorke bound is not compact either, due to a loss of regularity in the flow direction of a more elementary origin (see Lemma 4.1), which also played a part in Liverani's [30] proof. Like in [30], we may overcome these problems because we work with the resolvent R(z) = ∞ 0 e −zt L t dt which involves integration along the time direction.…”
Section: Contentsmentioning
confidence: 99%
See 3 more Smart Citations