2011
DOI: 10.4007/annals.2011.174.1.10
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Nonuniform measure rigidity

Abstract: Abstract. We consider an ergodic invariant measure µ for a smooth action α of Z k , k ≥ 2, on a (k + 1)-dimensional manifold or for a locally free smooth action of R k , k ≥ 2 on a (2k + 1)-dimensional manifold. We prove that if µ is hyperbolic with the Lyapunov hyperplanes in general position and if one element in Z k has positive entropy, then µ is absolutely continuous. The main ingredient is absolute continuity of conditional measures on Lyapunov foliations which holds for a more general class of smooth ac… Show more

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Cited by 31 publications
(49 citation statements)
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“…So we only consider the case (2). In that case, unless the entropy function is identically zero, the measure µ is absolutely continuous [7]. To summarize, the (deep) results of [7] and the above arguments provide the following dichotomy for ergodic invariant measures for maximal rank actions of rank k ≥ 2:…”
Section: Algebraic Actions and Rigidity Of The Fried Averagementioning
confidence: 92%
“…So we only consider the case (2). In that case, unless the entropy function is identically zero, the measure µ is absolutely continuous [7]. To summarize, the (deep) results of [7] and the above arguments provide the following dichotomy for ergodic invariant measures for maximal rank actions of rank k ≥ 2:…”
Section: Algebraic Actions and Rigidity Of The Fried Averagementioning
confidence: 92%
“…The theory, however, was not developed for quite a while. The linearization of a C 1+α diffeomorphism along a one-dimensional nonuniformly contracting foliation was constructed in [KKt07] and used in the study of measure rigidity in [KKt07,KKtR11]. Similar results for higher dimensional foliations with pinched exponents were obtained by Katok and Rodriguez Hertz in [KtR15].…”
Section: Introductionmentioning
confidence: 89%
“…Remark 3.2. In Kalinin, Katok and Hertz's paper [7] which investigates the nonuniform measure rigidity for Z k -actions, Lyapunov exponents for a Z k action on M are extended to a R k action on the suspension manifold S, which is a bundle over T k with fiber M . We can see that for any v = (v 1 , · · · , v k ) ∈ S k−1 , the Lyapunov exponents χ j ( v) in Proposition 2.1 of [7] is just the direction Lyapunov exponents λ v j in our case.…”
Section: Directional Lyapunov Exponents and Directional Entropymentioning
confidence: 99%