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“…Now, consider any countable set {x n } ⊂ supp µ such that the balls of radius δ/2 around these x n cover the support of µ. For each n, let B n be a zero µ-measure subset of the ball V (x n ) of radius δ around x n such that (29) m w = (h s z,w ) * m z for all z, w ∈ V (x n ) \ B n in the same stable piece. Let E be the set of all point x ∈ supp µ whose orbits never meet ∪ n B n and such that (30) m f l (x) = (F l x ) * m x for all l ∈ Z.…”
Section: 4mentioning
confidence: 99%
“…So, by Proposition 4.4, the two points z = f k (x) and w = f k (y) belong to the same stable piece (associated to x n ). Since they are outside B n , we may combine (29) and (30) with property (sh2) of s-holonomies to conclude that m y = (h s x,y ) * m x . This proves that the disintegration of m is essentially s-invariant, as claimed.…”
Section: 4mentioning
confidence: 99%
“…When the vectors in the center bundle E c also have non-zero Lyapunov exponents, that is, when lim 1 n log Df n (x)v = 0 ∀v ∈ E c x at typical points x ∈ M , one can build on (non-uniform) hyperbolicity theory to derive important geometric and statistical information on the dynamics. See Pesin [38,39], Ledrappier, Young [32,34,35], Katok [29], Barreira, Pesin, Schmeling [8], Young [45,46], and Alves, Bonatti, Viana [2,15].…”
Abstract. We propose a new approach to analyzing dynamical systems that combine hyperbolic and non-hyperbolic ("center") behavior, e.g. partially hyperbolic diffeomorphisms. A number of applications illustrate its power.We find that any ergodic automorphism of the 4-torus with two eigenvalues in the unit circle is stably Bernoulli among symplectic maps. Indeed, any nearby symplectic map has no zero Lyapunov exponents, unless it is volume preserving conjugate to the automorphism itself. Another main application is to accessible skew-product maps preserving area on the fibers. We prove, in particular, that if the genus of the fiber is at least 2 then the Lyapunov exponents must be different from zero and vary continuously with the map.These, and other dynamical conclusions, originate from a general Invariance Principle we prove in here. It is formulated in terms of smooth cocycles, that is, fiber bundle morphisms acting by diffeomorphisms on the fibers. The extremal Lyapunov exponents measure the smallest and largest exponential rates of growth of the derivative along the fibers. The Invariance Principle states that if these two numbers coincide then the fibers carry some amount of structure which is transversely invariant, that is, invariant under certain canonical families of homeomorphisms between fibers.
“…Now, consider any countable set {x n } ⊂ supp µ such that the balls of radius δ/2 around these x n cover the support of µ. For each n, let B n be a zero µ-measure subset of the ball V (x n ) of radius δ around x n such that (29) m w = (h s z,w ) * m z for all z, w ∈ V (x n ) \ B n in the same stable piece. Let E be the set of all point x ∈ supp µ whose orbits never meet ∪ n B n and such that (30) m f l (x) = (F l x ) * m x for all l ∈ Z.…”
Section: 4mentioning
confidence: 99%
“…So, by Proposition 4.4, the two points z = f k (x) and w = f k (y) belong to the same stable piece (associated to x n ). Since they are outside B n , we may combine (29) and (30) with property (sh2) of s-holonomies to conclude that m y = (h s x,y ) * m x . This proves that the disintegration of m is essentially s-invariant, as claimed.…”
Section: 4mentioning
confidence: 99%
“…When the vectors in the center bundle E c also have non-zero Lyapunov exponents, that is, when lim 1 n log Df n (x)v = 0 ∀v ∈ E c x at typical points x ∈ M , one can build on (non-uniform) hyperbolicity theory to derive important geometric and statistical information on the dynamics. See Pesin [38,39], Ledrappier, Young [32,34,35], Katok [29], Barreira, Pesin, Schmeling [8], Young [45,46], and Alves, Bonatti, Viana [2,15].…”
Abstract. We propose a new approach to analyzing dynamical systems that combine hyperbolic and non-hyperbolic ("center") behavior, e.g. partially hyperbolic diffeomorphisms. A number of applications illustrate its power.We find that any ergodic automorphism of the 4-torus with two eigenvalues in the unit circle is stably Bernoulli among symplectic maps. Indeed, any nearby symplectic map has no zero Lyapunov exponents, unless it is volume preserving conjugate to the automorphism itself. Another main application is to accessible skew-product maps preserving area on the fibers. We prove, in particular, that if the genus of the fiber is at least 2 then the Lyapunov exponents must be different from zero and vary continuously with the map.These, and other dynamical conclusions, originate from a general Invariance Principle we prove in here. It is formulated in terms of smooth cocycles, that is, fiber bundle morphisms acting by diffeomorphisms on the fibers. The extremal Lyapunov exponents measure the smallest and largest exponential rates of growth of the derivative along the fibers. The Invariance Principle states that if these two numbers coincide then the fibers carry some amount of structure which is transversely invariant, that is, invariant under certain canonical families of homeomorphisms between fibers.
“…Recall that the entropy of an Anosov flow is a measure of the growth rate of the lengths of the closed orbits of the flow [38]. Comparing the formulas (19) and (20) suggests that the term Def (g) should be viewed as a type of "mean variation" of the distribution of the closed orbits.…”
Abstract. In this paper we prove that for an ergodic hyperbolic measure ω of a C 1+α diffeomorphism f on a Riemannian manifold M , there is an ω-full measured set Λ such that for every invariant probability µ ∈ M inv ( Λ, f ), the metric entropy of µ is equal to the topological entropy of saturated set Gµ consisting of generic points of µ:hµ(f ) = htop(f, Gµ).
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