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Rigidity of Lyapunov exponents for derived from Anosov diffeomorphisms

Published online by Cambridge University Press:  14 October 2024

J. SANTANA COSTA
Affiliation:
DEMAT-UFMA, São Luis, MA, Brazil (e-mail: [email protected])
A. TAHZIBI*
Affiliation:
Departamento de Matemática, ICMC-USP, São Carlos, SP, Brazil
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Abstract

For a class of volume-preserving partially hyperbolic diffeomorphisms (or non-uniformly Anosov) $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ homotopic to linear Anosov automorphism, we show that the sum of the positive (negative) Lyapunov exponents of f is bounded above (respectively below) by the sum of the positive (respectively negative) Lyapunov exponents of its linearization. We show this for some classes of derived from Anosov (DA) and non-uniformly hyperbolic systems with dominated splitting, in particular for examples described by Bonatti and Viana [SRB measures for partially hyperbolic systems whose central direction is mostly contracting. Israel J. Math. 115(1) (2000), 157–193]. The results in this paper address a flexibility program by Bochi, Katok and Rodriguez Hertz [Flexibility of Lyapunov exponents. Ergod. Th. & Dynam. Sys. 42(2) (2022), 554–591].

Type
Original Article
Copyright
© The Author(s), 2024. Published by Cambridge University Press

1. Introduction

The Lyapunov exponents come from the study of differential equations in the thesis of Lyapunov [Reference Lyapunov14]. They were systematically introduced into ergodic theory by works of Furstenberg and Kesten [Reference Furstenberg and Kesten11] and Oseledets [Reference Oseledec18]. They are directly related to the expansion rates of the system and also to the positive metric entropy, using for example the Margulis–Ruelle inequality and the Pesin entropy formula. Ya. Pesin explored the concept of Lyapunov exponents developing a rich theory of non-uniformly hyperbolic systems, which are the systems with non-zero Lyapunov exponents.

However, in general, these systems are not robust: they do not form an open set. In the works [Reference Bochi3, Reference Bochi and Viana5], the authors show that if a non-uniformly hyperbolic system does not admit dominated splitting, it can be approximated by systems with zero Lyapunov exponents in $C^1$ topology. Usually, the presence of dominated decomposition guarantees higher regularity in $C^1$ topology, see for example [Reference Saghin, Valenzuela-Henríquez and Vásquez21]. In the non-invertible setting, [Reference Andersson, Carrasco and Saghin1] showed the existence of $C^1$ open sets without dominated decomposition such that integrated Lyapunov exponents vary continuously with the dynamics in the $C^1$ topology.

For a linear Anosov automorphism of the torus $A \colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ , the Lyapunov exponents are constant and indeed they are equal to the logarithm of the norm of eigenvalues of A. In general, Lyapunov exponents cannot be explicitly calculated. The regularity of Lyapunov exponents with respect to dynamics and invariant measures is a subtle question. Let us recall a flexibility conjecture by J. Bochi, A. Katok and F. Rodriguez Hertz. Let $\operatorname {Diff}_m^{\infty } (M)$ be the set of m-preserving diffeomorphisms (volume preserving) $f : M \rightarrow M$ of class  $C^{\infty }$ .

Conjecture 1.1. [Reference Bochi, Katok and Rodriguez Hertz4]

Given a connected component $C \subset \operatorname {Diff}_m^{\infty } (M)$ and any list of numbers $\xi _1 \geq \cdots \geq \xi _d$ with $\sum _{i=1}^{d} \xi _i =0,$ there exists an ergodic diffeomorphism $f \in C$ such that $\xi _i, i=1, \ldots , d$ are the Lyapunov exponents with respect to $m.$

Moreover, in the setting of volume-preserving Anosov diffeomorphisms, they posed the following problem.

Problem 1. [Reference Bochi, Katok and Rodriguez Hertz4]

(Strong flexibility) Let $A \in SL(d, \mathbb {Z})$ be a hyperbolic linear transformation inducing conservative Anosov diffeomorphism $F_A$ on $\mathbb {T}^d$ with Lyapunov exponents: $\unicode{x3bb} _1 \geq \unicode{x3bb} _2 \cdots \geq \unicode{x3bb} _{u}> 0 > \unicode{x3bb} _{u+1} \geq \cdots \geq \unicode{x3bb} _d.$ Given any list of numbers $\xi _1 \geq \xi _2 \geq \cdots \geq \xi _u \geq \xi _{u+1} \geq \cdots \geq \xi _d$ such that:

  1. (1) $\sum _{i=1}^{d} \xi _i = 0;$

  2. (2) $\sum _{i=1}^{u} \xi _i \leq \sum _{i=1}^{u} \unicode{x3bb} _i,$

does there exist a conservative Anosov diffeomorphism f homotopic to $F_A$ such that $\{\xi _i\}$ is the list of all Lyapunov exponents with respect to volume measure?

In this work, we study a subset of transformations $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ homotopic to a linear Anosov automorphism $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ , where f has some hyperbolicity (partial hyperbolicity or non-uniform hyperbolicity). See §2 for the definitions. In particular, we show that for a class of partially hyperbolic diffeomorphisms and homotopic to Anosov linear automorphism, not all lists of numbers can be realized as Lyapunov exponents. More precisely, in such a class of dynamics, we need the conditions (1) and (2) imposed in Problem 1.

This type of result also appears in [Reference Bochi, Katok and Rodriguez Hertz4, Reference Costa and Micena10, Reference Micena15Reference Micena and Tahzibi17, Reference Saghin and Xia22]. In [Reference Micena and Tahzibi16], it has been proved that for any conservative partially hyperbolic systems in the torus ${\mathbb {T}}^3$ , the stable or unstable Lyapunov exponent is bounded by the stable or unstable Lyapunov exponent of its linearization. It is well worth mentioning that Carrasco and Saghin [Reference Carrasco and Saghin9] constructed a $C^\infty $ and volume-preserving example on $\mathbb {T}^3$ that shows that the largest Lyapunov exponent of a diffeomorphism in the homotopy class of an Anosov linear automorphism of $\mathbb {T}^3$ may be larger than the largest Lyapunov exponent of A. However, in their example, f does not admit a three-bundle partially hyperbolic splitting.

We also mention that our results address (and give a negative answer in some special cases of derived from Anosov diffeomorhisms) a question in [Reference Carrasco and Saghin9]: Does there exist a derived from Anosov diffeomorphism f such that the sum of the positive Lyapunov exponents of f is larger than the sum of the positive Lyapunov exponents of its linear part?

2. Definitions and statements of results

Definition 2.1. Let M be a closed manifold. A diffeomorphism $f\colon M \rightarrow M$ is called a partially hyperbolic diffeomorphism if there is a suitable norm $\|\cdot \|$ and the tangent bundle $TM$ admits a $Df$ -invariant decomposition $TM = E^s \oplus E^c \oplus E^u$ such that for all unitary vectors $v^{\sigma } \in E^{\sigma }_x, \sigma \in \{s,c,u\}$ and every $x \in M$ , we have

$$ \begin{align*} \|D_x f v^s \| < \|D_x f v^c \| < \|D_x f v^u \|;\end{align*} $$

moreover,

$$ \begin{align*}\|D_x f v^s \| < 1 \quad\text{and}\quad \|D_x f v^u \|> 1 .\end{align*} $$

Every diffeomorphism of the torus $\mathbb {T}^d$ induces an automorphism of the fundamental group and there exists a unique linear diffeomorphism $f_{\ast }$ which induces the same automorphism on $\pi _1(\mathbb {T}^d).$ The diffeomorphism $f_{\ast }$ is called linearization of $f.$

Anosov diffeomorphisms can be considered partially hyperbolic systems with $E^c = 0.$ However, in this paper, whenever we consider an Anosov diffeomorphism as a partially hyperbolic system, we mean that there exists a non-trivial (centre bundle) partially hyperbolic decomposition.

Clearly, a partially hyperbolic diffeomorphism may have various partially hyperbolic invariant decompositions. We will consider several (non-necessarily disjoint) categories of partially hyperbolic diffeomorphisms indexed by the dimensions of invariant bundles.

More precisely, we say $f \in Ph_{(d_s, d_u)}(M)$ if f admits a partially hyperbolic decomposition with $\dim (E^{\sigma }) = d_{\sigma }$ for $ \sigma \in \{s, u\}.$ Clearly, $\dim (E^c) = \dim (M) - d_s - d_u.$ For instance, consider the cat map A on $\mathbb {T}^2$ induced by matrix $(\begin {smallmatrix} 2 & 1 \\ 1 & 1 \\ \end {smallmatrix} )$ , then $A \times A$ is a partially hyperbolic (in fact, Anosov) diffeomorphism and belongs to $Ph_{(1, 1)} \cap Ph_{(2,1)} \cap Ph_{(1, 2)}.$

Definition 2.2. Let $f\colon \mathbb {T}^d \rightarrow \mathbb {T}^d $ be a partially hyperbolic diffeomorphism, and f is called a derived from Anosov (DA) diffeomorphism if its linearization $f_{\ast }\colon \mathbb {T}^d \rightarrow \mathbb {T}^d $ is a linear Anosov automorphism.

Definition 2.3. We say that the diffeomorphism $f\colon M\rightarrow M$ admits a dominated splitting if there is an invariant (by $Df$ ) continuous decomposition $TM=E\oplus F$ and constants $0<\nu <1, C>0$ such that

$$ \begin{align*} \frac{\|Df^n|_{E(x)}\|}{\|Df^{-n}|_{F(f^n(n))}\|^{-1}}\leq C\nu^n\quad\text{for all } x\in M, n>0. \end{align*} $$

Let us recall a simple version of the Oseledets’ theorem.

Theorem 2.4. [Reference Oseledec18]

Let $f\colon M\rightarrow M$ be a $C^1$ diffeomorphism, then there is a full probability Borelian set $\mathcal {R}$ (this is, $\mu (\mathcal {R})=1$ for all f-invariant probability measure $\mu $ ) such that for each $x\in \mathcal {R}$ , there is a decomposition $T_xM=E_1\oplus \cdots E_{k(x)}$ and constants $\unicode{x3bb} _1,\ldots ,\unicode{x3bb} _{k(x)}$ such that

for all $v\in E_i$ . The $\unicode{x3bb} _i(x)$ is called a Lyapunov exponent. Moreover, for any $ 1 \leq j \leq k(x) $ ,

where $F_j = E_1 \oplus \cdots \oplus E_j$ and $d_i= \mathrm {dim} (E_i).$

In this paper, when m refers to a measure, it stands for a fixed Lebesgue measure on $\mathbb {T}^d$ .

2.1. Lyapunov exponents of partially hyperbolic diffeomorphisms

In our first main theorem, we prove that linear Anosov diffeomorphisms maximize (respectively minimize) the sum of unstable (respectively stable) Lyapunov exponents, in any homotopy path totally inside partially hyperbolic diffeomorphisms.

The notion of metric entropy appears naturally when dealing with Lyapunov exponents. For a partially hyperbolic diffeomorphism, it is possible to define entropy of an invariant measure along unstable foliation and there is variational principle results for such entropy. A u-maximal entropy measure is a measure which attains the supremum of unstable entropy among all invariant measures. See §3.2.1 and references for more details.

Theorem A. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a $C^2$ volume-preserving DA diffeomorphism in $Ph_{d_s, d_u}$ with linearization $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ such that f and A are homotopic by a path fully contained in $Ph_{d_s, d_u}({\mathbb {T}}^d)$ , then

$$ \begin{align*} \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(f, x) \leq \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(A) \,\,\,\, \text{and} \,\,\,\, \sum_{i = 1}^{d_s} \unicode{x3bb}^s_i(f, x) \geq \sum_{i = 1}^{d_s} \unicode{x3bb}^s_i(A), \end{align*} $$

for m-almost every (a.e.) $x \in {\mathbb {T}}^d$ and, the first (respectively second) inequality is strict unless m is a measure of u-maximal entropy (respectively u-maximal for $f^{-1}$ ).

This is related to the result of [Reference Micena and Tahzibi16]: let $f\colon \mathbb {T}^3 \rightarrow \mathbb {T}^3$ be a $C^2$ conservative derived from Anosov partially hyperbolic diffeomorphism with linearization A. Then, $\unicode{x3bb} ^u(x) \leq \unicode{x3bb} ^u(A)$ for almost every $x.$ We recall that the authors used quasi-isometric property of unstable foliation for the three-dimensional derived from Anosov diffeomorphisms. They do not assume that f is in the same connected component of A.

Theorem B. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a $C^2$ volume-preserving DA diffeomorphism in $Ph_{d_s, d_u}$ with linearization $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ belonging to $Ph_{d_s, d_u}.$ Suppose that for $\sigma \in \{s, u\}$ , there is a $(d - d_{\sigma })$ -dimensional subspace $P_{\sigma } \subset \mathbb {R}^d, $ such that $\angle (E^{\sigma }_f(x), P_{\sigma })> \alpha > 0$ for all $x \in \mathbb {R}^d$ ( $E^{\sigma }_f$ stands for the lift of the bundles), then

$$ \begin{align*} \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(f, x) \leq \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(A) \quad \text{and} \quad \sum_{i = 1}^{d_s} \unicode{x3bb}^s_i(f, x) \geq \sum_{i = 1}^{d_s} \unicode{x3bb}^s_i(A), \end{align*} $$

for m-a.e. $x \in \mathbb {T}^d.$

Observe that the assumption on the existence of $P_{\sigma }$ in the above theorem is a mild condition and is satisfied if the stable and unstable bundles of f do not vary too much. Indeed, we require that $\{ E^{\sigma }_f(x), x \in \mathbb {R}^d\}$ is not dense in the Grassmannian of $d_{\sigma }$ -dimensional subspaces.

2.2. Lyapunov exponents of non-uniformly Anosov systems

In this section, we deal with dynamics that are not necessarily partially hyperbolic. However, they enjoy some dominated splitting property: Oseledets’ splitting (stable/unstable) is dominated.

Definition 2.5. A $C^2$ -volume-preserving diffeomorphism f is called non-uniformly Anosov if it admits an f-invariant dominated decomposition $TM= E \oplus F$ such that $\unicode{x3bb} ^{F}_i(x)>0$ (all Lyapunov exponents along F) and $\unicode{x3bb} ^{E}_i(x)<0$ (all Lyapunov exponents along E) for $\mu $ -a.e x.

In the next theorem, we compare Lyapunov exponents of a non-uniformly Anosov diffeomorphism with those of linear Anosov automorphism if they are homotopic. Observe that by definition, the number of negative (positive) Lyapunov exponents of a non-uniformly Anosov diffeomorphism is constant almost everywhere and coincides with the dimension of the bundles in the dominated splitting. However, the Lyapunov exponents may depend on the orbit, as we do not assume ergodicity. In fact, it is interesting to know whether, in general, all topologically transitive non-uniformly Anosov diffeomorphisms are ergodic or not. We conjecture that all topologically transitive non-uniformly Anosov diffeomorphisms are ergodic.

Let $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a linear Anosov diffeomorphism such that $T \mathbb {T}^d = E^s_{A} \oplus E^u_{A}.$ Denote by $d_s =\mathrm {dim} (E^s_A)$ and $d_u =\mathrm {dim}(E^u_A).$ After changing to an equivalent Riemannian norm, if necessary, there are $0<\unicode{x3bb} <1<\gamma $ such that $\|A|_{E^s}\| \leq \unicode{x3bb} $ , $m(A|_{E^u}) \geq \gamma $ and $E^s_A$ is orthogonal to $E^u_A.$ Indeed, to use fewer constants in the proofs, we assume that $E^u_i$ and $E^u_j, i \neq j$ are orthogonal, where $E^u_i$ terms are generalized eigenspaces of A which coincide with the Oseledets decomposition. Recall that for a linear transformation T, $m(T):= \|T^{-1}\|^{-1}.$ We refer to $\gamma , \unicode{x3bb} $ as rates of hyperbolicity of A. Observe that Lyapunov exponents of any diffeomorphism are independent of the choice of the equivalent norm.

Theorem C. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a $C^{2}$ conservative non-uniformly Anosov diffeomorphism with dominated decomposition $TM=E\oplus F$ , homotopic to A such that:

  1. (1) $\mathrm {dim} (E) =d_s$ and $\mathrm {dim} (F) =d_u;$

  2. (2) $E(x)\cap E^u_A=\{0\}$ and $F(x)\cap E^s_A=\{0\};$

  3. (3) $\|Df|_E\|<\gamma $ and $m(Df|_F)>\unicode{x3bb} $ .

Suppose that the distributions E and F are integrable, then $\sum _{i=1}^{d_u}\unicode{x3bb} ^{F}_{i}(f,x)\leq \sum _{i=1}^{d_u}\unicode{x3bb} _i^u(A)$ and $\sum _{i=1}^{d_s}\unicode{x3bb} ^{E}_i(f,x)\geq \sum _{i=1}^{d_s} \unicode{x3bb} _i^s(A)$ for Lebesgue-a.e. $x\in {\mathbb {T}}^d$ .

Let us comment on the hypotheses: the first and second one ask for some compatibility of invariant bundles and the third one asks that any possible expansion in the dominated bundle E is less than the expansion rate of A and similarly any possible contraction in the dominating bundle F is weaker than the contraction rate of $A.$

Bonatti and Viana [Reference Bonatti and Viana6] constructed the first examples of robustly transitive diffeomorphisms that are not partially hyperbolic, which was later generalized in higher dimensions by [Reference Tahzibi23]. Those classes of examples satisfy the hypotheses of the above theorem.

Theorem 2.6. [Reference Bonatti and Viana6, Reference Buzzi and Fisher8, Reference Tahzibi23]

There is an open set $\mathcal {U}\subset \operatorname {Diff}^1_m({\mathbb {T}}^d)$ such that any $C^2$ -diffeomorphism in $\mathcal {U}$ satisfies all hypotheses of Theorem C and the bundles E and F are integrable.

In the above theorem, the integrability of invariant subbundles E and F is proved in [Reference Buzzi and Fisher8].

2.3. Regularity of foliations

Any partially hyperbolic diffeomorphism admits invariant stable and unstable foliations. As the proofs of our main results are based on the regularity of such foliations, we need to recall some basic definitions and results in this subsection. Consider ${\mathcal {F}}$ a foliation in M, B a ${\mathcal {F}}$ -foliated box and m the Lebesgue measure in M. Denote by $\mathrm {Vol}_{L_x}$ the Lebesgue measure of leaf $L_x$ and $m_{L_x}$ the disintegration of the Lebesgue measure m along the leaf $L_x$ . The disintegrated measures are in fact a projective class of measures. However, whenever we fix a compact foliated box B, then we can use the Rohlin disintegration theorem for the normalized restriction of m on B to get probability conditional measures. So in what follows, after fixing a foliated box B by $m_{L_x}$ and $\mathrm {Vol}_{L_x}$ , we understand probability measures whose support is inside the plaque of $L_x$ which contains $x \in B$ and is inside B.

Definition 2.7. We say that the foliation ${\mathcal {F}}$ is upper leafwise absolutely continuous if for any foliated box B, $m_{L_x}\!\ll \mathrm {Vol}_{L_x}$ for m-a.e. $x\in B$ . Equivalently, if given a set $Z\subset B$ such that $\mathrm {Vol}_{L_x}(Z\cap L_x)=0$ for m-a.e. $x \in B$ , then $m(Z)=0$ .

Definition 2.8. We say that the foliation ${\mathcal {F}}$ is lower leafwise absolutely continuous if $\mathrm {Vol}_{L_x}\!\ll m_{L_x}$ for m-a.e. $x\in B$ . Equivalently, if given a set $Z\subset B$ such that $m(Z)=0$ , then $\mathrm {Vol}_{L_x}(Z\cap L_x)=0$ for m-a.e. $x \in B$ .

Definition 2.9. We say that the foliation ${\mathcal {F}}$ is leafwise absolutely continuous if $\mathrm {Vol}_{L_x}\!\sim m_{L_x}$ (this is, $m_{L_x}\!\ll \mathrm {Vol}_{L_x}$ and $\mathrm {Vol}_{L_x}\!\ll m_{L_x}$ ) for m-a.e. $x\in B$ .

Proposition 2.10. [Reference Brin and Pesin7]

If $f\colon M\rightarrow M$ is a $C^2$ partially hyperbolic diffeomorphism, then the foliations $W^s$ and $W^u$ are leafwise absolutely continuous.

We also mention the result of Ya. Pesin for non-uniformly hyperbolic systems, see [Reference Barreira and Pesin2, Theorem 4.3.1], which shows absolute continuity of local Pesin laminations.

3. Proof of results

Theorems A and B are obtained by the following result.

Theorem 3.1. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a $C^2$ volume-preserving partially hyperbolic diffeomorphism such that there are closed non-degenerate $d_u$ -forms and $d_s$ -forms on $E^u$ and $E^s$ , respectively. Suppose that A, the linearization of f, is partially hyperbolic and $\mathrm {dim} E^{\sigma }_f=\mathrm {dim} E^{\sigma }_A$ , $\sigma \in \{s,c,u\}$ , then

for m-a.e. $x\in {\mathbb {T}}^d$ .

For the proof of this theorem, we use a result of Saghin [Reference Saghin20]. Let $f\colon M\rightarrow M$ be a diffeomorphism and W an f-invariant foliation on M, that is, $f(W(x))=W(f(x))$ , and $B_r(x,f)$ be the ball of the leaf $W(x)$ with radius r centred at x. We say that

$$ \begin{align*} \chi_W(f,x)=\limsup_{n\rightarrow\infty}\frac{1}{n}\log \mathrm{Vol}(f^n(B_r(x,f))) \end{align*} $$

is the volume growth rate of the foliation at x and

$$ \begin{align*} \chi_W(f)=\sup_{x\in M}\chi_W(f,x) \end{align*} $$

is the volume growth rate of W. Here, Vol stands for the $\mathrm {Vol}_{W}$ which is the induced volume to the leaves of W. We use this notation throughout the paper except when it may create confusion.

When f is a partially hyperbolic diffeomorphism, we denote by $\chi _u(f)$ the volume growth of unstable foliation $W^u$ .

Theorem 3.2. [Reference Saghin20]

Let $f\colon M\rightarrow M$ be a $C^1$ partially hyperbolic diffeomorphism such that there is a closed non-degenerate $d_u$ -form on the unstable bundle $E^u$ , then $\chi _u(f)=\log sp(f_{*,d_u})$ , where $f_{*,d_u}$ is the induced map in the $d_u$ -cohomology of De Rham.

Proposition 3.3. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a $C^1$ partially hyperbolic diffeomorphism admitting a closed non-degenerate $d_u$ -form on the unstable bundle $E^u$ . For fixed ${x\in {\mathbb {T}}^d, r>0}$ , the balls $B_r(x,f)\subset W^u(x,f)$ and $B_r(x,A)\subset W^u(x,A)$ satisfy the following. Given $\varepsilon>0$ , there is $n_0 \in \mathbb {N}$ such that if $n>n_0$ , we have

$$ \begin{align*} \mathrm{Vol}_{W^u(f)}(f^n(B_r(x,f)))\leq(1+\varepsilon)^n\mathrm{Vol}_{W^u(A)}(A^n(B_r(x,A))). \end{align*} $$

Proof. By Theorem 3.2, we have that

$$ \begin{align*} \chi_u(f,x)\leq\chi_u(f)=\log sp(f_{*,u})=\log sp(A_{*,u})=\chi_u(A)=\chi_u(A,x), \end{align*} $$

that is,

$$ \begin{align*} \limsup_{n\rightarrow\infty}\frac{1}{n}\log \mathrm{Vol}_{W^u(f)}(f^n(B_r(x,f)))\leq \lim_{n\rightarrow\infty}\frac{1}{n}\log \mathrm{Vol}_{W^u(A)}(A^n(B_r(x,A))); \end{align*} $$

therefore, given $\varepsilon>0$ , there is $n_0$ such that if $n>n_0$ ,

$$ \begin{align*} \frac{1}{n}\log \mathrm{Vol}_{W^u(f)}(f^n(B_r(x,f)))\leq \frac{1}{n}\log \mathrm{Vol}_{W^u(A)}(A^n(B_r(x,A)))+\frac{1}{n}\log (1+\varepsilon)^n. \end{align*} $$

Then,

$$ \begin{align*} \mathrm{Vol}_{W^u(f)}(f^n(B_r(x,f)))\leq(1+\varepsilon)^n\mathrm{Vol}_{W^u(A)}(A^n(B_r(x,A))).\\[-37pt] \end{align*} $$

Proof of Theorem 3.1

We prove the statement for the sum of unstable exponents. One may repeat the argument for $f^{-1}$ to obtain the claim for stable exponents.

Suppose by contradiction that there is a positive volume set $Z\subset \mathcal {R} \subset {\mathbb {T}}^d$ , (where $\mathcal {R}$ is the set of points satisfying Oseledets’ theorem as stated in Theorem 2.4) such that for all $x\in Z$ , we have $\sum _{i=1}^{d_u}\unicode{x3bb} ^u_i(f,x)>\sum _{i=1}^{d_u}\unicode{x3bb} ^u_i(A)$ .

For $q\in {\mathbb {N}}\setminus \{0\}$ , we define the set

Since $\bigcup _{q=1}^{\infty }Z_q=Z$ , there is a q such that $m(Z_q)>0$ . For any $x\in Z_q$ , we have

So, there is $n_0$ such that for $n\geq n_0$ , we have

So we get

By this fact, for each $n>0$ , we define the set

So, there is $N>0$ with $m(Z_{q,N})>0$ .

Now for any $x\in {\mathbb {T}}^d$ , let $B_x$ be a foliated box of $W^u_{f}$ around x. By compactness, we can take a finite cover $\{B_{x_i}\}_{i=1}^{j}$ of ${\mathbb {T}}^d$ . As $W^u_f$ is absolutely continuous [Reference Brin and Pesin7], there is i and $x\in B_{x_i}$ such that $\mathrm {Vol}_ W^u(f)(B_{x_i}\cap W^u_{f}(x)\cap Z_{q,N})>0$ .

Consider $B_r(x)\subset W^u_f(x)$ satisfying $ {\mathrm {Vol}_{W^u(f)}(B_r(x)\cap Z_{q,N})>0}$ . By Proposition 3.3, there is $K(\epsilon ) \in \mathbb {N}$ such that for all $k \geq K(\epsilon )$ ,

(3.1) $$ \begin{align} \mathrm{Vol}_{W^u(f)}(f^k(B_r(x)))&\leq (1+\epsilon)^k\mathrm{Vol}_{W^u(A)}(A^k(B_r(x)))\nonumber\\&\leq(1+\epsilon)^k e^{k\sum\unicode{x3bb}^u_i(A)}\mathrm{Vol}_{W^u(A)}(B_r(x)). \end{align} $$

However, for $k\geq N$ ,

(3.2)

Taking $\epsilon < {1}/{q},$ for large enough k, the inequalities in equations (3.1) and (3.2) give a contradiction.

3.1. Proof of Theorem B

We use Theorem 3.1 and the following proposition to conclude the proof of Theorem B.

Proposition 3.4. Let W be a foliation in ${\mathbb {R}}^d$ of dimension $d_u$ . If there is a ( $d\text {--}d_u$ )-plane P in ${\mathbb {R}}^d$ such that $\angle (T_xW,P)>\alpha >0$ for all $x\in {\mathbb {R}}^d$ , then there is a $d_u$ -form $\omega $ which is closed and non-degenerate on W.

Proof. Let B be the orthogonal complement of P, there is always a closed and non-degenerate form in B, in fact, just take the volume form $\omega =dx_1\wedge dx_2\wedge \cdots \wedge dx_{d_u}$ which is non-degenerate in B and $\omega $ is closed. Note that $\omega $ is degenerate only in $B^{\bot }=P$ and by hypothesis, $\angle (T_xW,P)>\alpha >0$ . So, $\omega $ is closed and non-degenerate in $T_xW$ for all $x\in {\mathbb {R}}^d$ .

Corollary 3.5. If $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ is a linear partially hyperbolic diffeomorphism and f is a $C^2$ conservative diffeomorphism which is a small $C^1$ -perturbation of A, then $\sum _{i=1}^{d_u}\unicode{x3bb} _i^u(f,x)\leq \sum _{i=1}^{d_u}\unicode{x3bb} _i^u(A)$ and $\sum _{i=1}^{d_s}\unicode{x3bb} _i^s(f,x)\geq \sum _{i=1}^{d_s} \unicode{x3bb} _i^s(A)$ for Lebesgue-a.e. ${x\in {\mathbb {T}}^d}$ .

3.2. Proof of Theorem A

From [Reference Roldan19, Proposição 3.1.2], we have the following proposition.

Proposition 3.6. [Reference Roldan19]

Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a partially hyperbolic diffeomorphism homotopic to a linear Anosov diffeomorphism A such that:

  1. (a) each element of the homotopic path is a partially hyperbolic diffeomorphism;

  2. (b) if $f_1$ and $f_2$ are two elements of the homotopic path, then $\mathrm {dim} E^{\sigma }(f_1)=\mathrm {dim} E^{\sigma }(f_2)$ , $\sigma \in \{s,c,u\},$

then there exists a closed non-degenerate $d_u$ -form on $W^u(f)$ .

By the proposition above, f has a $d_u$ closed and non-degenerate form on $W^u$ , using the inverse $f^{-1}$ , we get a $d_s$ closed and non-degenerate form on $W^s$ . By Theorem 3.1, we conclude the first part of Theorem A. In the next subsection, we complete the proof.

3.2.1. Maximizing measures

In this section, we prove the last part of Theorem A. We write all proofs for the unstable bundle.

First, we recall the definition of topological and metric entropy along an expanding foliation. In [Reference Hu, Hua and Wu13], the authors define the notion of topological and metric entropy along unstable foliation and prove the variational principle.

Let $f\colon M\rightarrow M$ be a $C^1$ -partially hyperbolic diffeomorphism and $\mu $ is an f-invariant probability measure. For a partition $\alpha $ of M, denote $\alpha _0^{n-1}=\bigvee _{i=0}^{n-1}f^{-i}\alpha $ and by $\alpha (x)$ the element of $\alpha $ containing x. Given $\varepsilon>0$ , let $\mathcal {P}=\mathcal {P}_{\varepsilon }$ denote the set of finite measurable partitions of M whose elements have diameters smaller than or equal to $\varepsilon $ . For each $\alpha \in \mathcal {P}$ , we define a partition $\eta $ such that $\eta (x)=\alpha (x)\cap W^u_\mathrm{loc}(x)$ for each $x \in M$ , where $W^u_\mathrm{loc}(x)$ denotes the local unstable manifold at x whose size is greater than the diameter $\varepsilon $ of $\alpha $ . Let $\mathcal {P}^u=\mathcal {P}^u_{\varepsilon }$ denote the set of partitions $\eta $ obtained in this way. We define the conditional entropy of $\alpha $ given $\eta $ with respect to $\mu $ by

$$ \begin{align*} H_{\mu}(\alpha|\eta):=-\int_{M}\log\mu^{\eta}_{x}(\alpha(x))\,d\mu(x), \end{align*} $$

where $\mu ^{\eta }_{x}$ refer to the disintegration of $\mu $ along $\eta $ .

Definition 3.7. The conditional entropy of f with respect to a measurable partition $\alpha $ given $\eta \in \mathcal {P}^u$ is defined as

$$ \begin{align*} h_{\mu}(f,\alpha|\eta)=\limsup_{n\rightarrow \infty}\frac{1}{n}H_{\mu}(\alpha_{0}^{n-1}|\eta). \end{align*} $$

The conditional entropy of f given $\eta \in \mathcal {P}^u$ is defined as

$$ \begin{align*} h_{\mu}(f|\eta)=\sup_{\alpha\in\mathcal{P}}h_{\mu}(f,\alpha|\eta), \end{align*} $$

and the unstable metric entropy of f is defined as

$$ \begin{align*} h_{\mu}^u(f)=\sup_{\eta\in\mathcal{P}^u}h_{\mu}(f|\eta). \end{align*} $$

Now, we go to define the unstable topological entropy.

We denote by $\rho ^u$ the metric induced by the Riemannian structure on the unstable manifold and let $\rho ^u_n(x,y)=\max _{0\leq j\leq n-1}\rho ^u(f^j(x),f^j(y))$ . Let $W^u(x,\delta )$ be the open ball inside $W^u(x)$ centred at x of radius $\delta $ with respect to the metric $\rho ^u$ . Let $N^u(f,\epsilon ,n,x,\delta )$ be the maximal number of points in $\overline {W^u(x,\delta )}$ with pairwise $\rho ^u_ n$ -distances at least $\epsilon $ . We call such a set an $(n,\epsilon ) u$ -separated set of $\overline {W^u(x,\delta )}$ .

Definition 3.8. The unstable topological entropy of f on M is defined by

$$ \begin{align*} h^{u}_{\mathrm{top}}(f)=\lim_{\delta\to 0}\sup_{x\in M}h^u_{\mathrm{top}}(f,\overline{W^u(x,\delta)}), \end{align*} $$

where

$$ \begin{align*} h^u_{\mathrm{top}}(f,\overline{W^u(x,\delta)})=\lim_{\epsilon\to 0}\limsup_{n\to\infty}\frac{1}{n}\log N^u(f,\epsilon,n,x,\delta). \end{align*} $$

Let $\mathcal {M}_f(M)$ and $\mathcal {M}_f^e(M)$ denote the set of all f-invariant and ergodic probability measures on M, respectively.

Theorem 3.9. [Reference Hu, Hua and Wu13]

Let $f\colon M\rightarrow M$ be a $C^1$ -partially hyperbolic diffeomorphism. Then,

$$ \begin{align*} h^u_{\mathrm{top}}(f)=\sup\{h^u_{\mu}(f): \mu\in\mathcal{M}_f(M)\}. \end{align*} $$

Moreover,

$$ \begin{align*} h^u_{\mathrm{top}}(f)=\sup\{h^u_{\nu}(f): \nu\in\mathcal{M}_f^e(M)\}. \end{align*} $$

Furthermore, the authors proved that unstable topological entropy coincides with unstable volume growth.

Theorem 3.10. [Reference Hu, Hua and Wu13]

Unstable topological entropy coincides with unstable volume growth, i.e. $h^u_{\mathrm {top}}(f)=\chi _u(f)$ .

As in the hypotheses of Theorem A, the diffeomorphisms f and A are homotopic, so using Theorem 3.2, we have

$$ \begin{align*} h^u_{\mathrm{top}}(f)=\chi_u(f)=\log sp(f_{\ast},u)=\log sp(A_{\ast},u)=\chi_u(A)=h^u_{\mathrm{top}}(A). \end{align*} $$

Thus,

$$ \begin{align*} \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(f, x)=h^u_m(f)\leq h^u_{\mathrm{top}}(f)=h^u_{\mathrm{top}}(A)= \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(A). \end{align*} $$

Then we conclude that $h^u_m(f)= h^u_{\mathrm {top}}(f)$ .

3.3. Proof of Theorem C

We remember that $A\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ is a linear Anosov diffeomorphism and $0<\unicode{x3bb} <1<\gamma $ are rates for hyperbolicity, $d_s =\mathrm {dim} (E^s_A)$ and ${d_u =\mathrm {dim} (E^u_A).}$ Let $W^s_A, W^u_A$ be the stable and unstable foliation of A and by $\widetilde {W}^{s}_A$ , $\widetilde {W}^{u}_A$ , we denote their lifts to the universal cover $\mathbb {R}^d$ . These foliations are stable and unstable foliations of $\widetilde {A}$ which is a lift of A. We use ‘ $\sim $ ’ for objects in the universal cover. The norm and distance on $\mathbb {R}^d$ are the lift of adapted norm and corresponding distance where the hyperbolicity conditions of A are satisfied, see §2.2 before the announcement of Theorem C.

Similar to [Reference Hammerlindl12, Proposition 2.5 and Corollary 2.6], we show the following proposition.

Proposition 3.11. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a diffeomorphism that admits a dominated splitting $TM=E\oplus F$ with $\|Df|_E\|\leq \hat {\gamma }<\gamma $ and $m(Df|_F) \geq \hat {\unicode{x3bb} }>\unicode{x3bb} $ , homotopic to A such that $\mathrm {dim} (E) =d_s$ and $\mathrm {dim} (F) =d_u.$ Suppose that the distributions E and F are integrable, and denote by $\mathcal {E}$ and $\mathcal {F}$ their respective tangent foliations, then there is $R>0$ such that:

  • $\mathcal {E}(x)\subset B_{R}(\widetilde {W}^{s}_A(x))$ ;

  • $\mathcal {F}(x)\subset B_{R}(\widetilde {W}^{u}_A(x))$ ,

where $B_{R}(\widetilde {W}^{s}_A(x)) \subset \mathbb {R}^d$ is the set of points which are at distance R from $W^s_A(x)$ . Use a similar definition for $B_{R}(\widetilde {W}^{u}_A(x)).$

Corollary 3.12. Fixing $x \in \mathbb {R}^n$ , if $ \|x-y\|\rightarrow \infty $ and $y\in \mathcal {E}(x)$ , then $({x-y})/{\|x-y\|}\rightarrow \widetilde {E}^{s}_A(x)$ uniformly. More precisely, for $\varepsilon>0$ , there is $M>0$ such that if $x\in {\mathbb {R}}^d$ , $y\in \mathcal {E}(x)$ and $\|x-y\|>M$ , then

$$ \begin{align*} \|\pi_A^{u}(x-y)\|<\varepsilon\|\pi^{s}_A(x-y)\|, \end{align*} $$

where $\pi _A^{s}$ is the orthogonal projection on the subspace $E^s_A$ along $E^u_A$ , and $\pi _A^{u}$ is the projection on the subspace $E^{u}_A$ along $E^s_A.$

Analogous statements hold for $\mathcal {F}$ . The following proposition is a topological remark (see [Reference Hammerlindl12]) and comes from the fact that f and A are homotopic and A is not singular.

Proposition 3.13. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ be a homeomorphism with linearization A, then for each $k \in {\mathbb {Z}}$ and $C>1$ , there is an $M>0$ such that for all $x,y\in {\mathbb {R}}^d$ ,

$$ \begin{align*} \|x-y\|>M \Rightarrow \frac{1}{C}<\frac{\|\tilde{f}^k(x)-\tilde{f}^k(y)\|}{\|\tilde{A}^k(x)-\tilde{A}^k(y)\|}<C. \end{align*} $$

More generally, for each $k\in {\mathbb {Z}}$ , $C>1$ and any linear projection $\pi \colon {\mathbb {R}}^d\rightarrow {\mathbb {R}}^d$ , with A-invariant image, there is $M> 0$ such that for $x,y\in {\mathbb {R}}^d$ , with $\|x-y\|>M$ ,

$$ \begin{align*} \frac{1}{C}<\frac{\|\pi(\tilde{f}^k(x)-\tilde{f}^k(y))\|}{\|\pi(\tilde{A}^k(x)-\tilde{A}^k(y))\|}<C. \end{align*} $$

Proof of Proposition 3.11

To prove the first claim (the second one is similar), it is enough to show that $\|\pi ^u_A(x-y)\|$ is uniformly bounded for all $y\in \mathcal {E}(x)$ . Let $C>1$ close enough to $1$ such that $C \hat {\gamma } < \gamma $ and $1 < {\gamma }/{C}.$ Put $k=1$ and C chosen as above in Proposition 3.13, and get appropriate M. By contradiction, suppose that $\|\pi ^u_A(x-y)\|$ is not bounded. So, there is $y\in \mathcal {E}(x)$ with $\|\pi ^u_A(x-y)\|>M$ and consequently,

$$ \begin{align*} \|\pi^u_A(\tilde{f}(x)-\tilde{f}(y))\|> \frac{1}{C}\|\pi^u_A(\tilde{A}(x-y))\| = \frac{1}{C} \|(\tilde{A}( \pi^u_A(x-y))\| \geq \frac{\gamma}{C} \|\pi^u_A(x-y) \| > M, \end{align*} $$

which implies that we can use induction and for any $n \geq 1$ , obtain

$$ \begin{align*} \|\pi^u_A(\tilde{f}^{n}(x)-\tilde{f}^{n}(y))\|>\frac{\gamma^{n}}{C^n} M. \end{align*} $$

Finally, there is a constant $\eta> 0$ such that

(3.3) $$ \begin{align} \|\tilde{f}^{n}(x)-\tilde{f}^{n}(y)\|> \eta \frac{\gamma^{n}}{C^n} M. \end{align} $$

Now consider a smooth curve $\alpha \colon [a,b]\rightarrow \mathcal {E}(x)$ with $\alpha (a)=x$ and $\alpha (b)=y$ whose length is $d_{\mathcal {E}}(x,y)$ . Then,

$$ \begin{align*} \|\tilde{f}^{n}(x)-\tilde{f}^{n}(y)\|&\leq d_{\mathcal{E}}(\tilde{f}^{n}(x),\tilde{f}^{n}(y))\leq l(\tilde{f}^{n}(\alpha(t))) =\int_a^b\bigg\|\frac{d}{dt}(\tilde{f}^{n}(\alpha(t))\bigg\|\,dt\\ &\leq \int_a^b\|D\tilde{f}^{n}|_{W^{cs}}\|\cdot\|(\alpha'(t))\|\,dt< \int_a^b\hat{\gamma}^{n} \|\alpha'(t)\|\,dt, \end{align*} $$

implies that

(3.4) $$ \begin{align} \|\tilde{f}^{n}(x)-\tilde{f}^{n}(y)\|<\hat{\gamma}^{n}\,d_{\mathcal{E}}(x,y). \end{align} $$

Equations (3.3) and (3.4) and ${\gamma }/{C}> \hat {\gamma }$ give us a contradiction when n is large enough.

Proposition 3.14. Let $f\colon M\rightarrow M$ be a $C^2$ conservative non-uniformly Anosov diffeomorphism with $TM = E \oplus F$ . If the distribution E is integrable, then the respective foliation $\mathcal {E}$ is upper leafwise absolutely continuous.

Let $\mathcal {R}$ be the regular set in Pesin sense such that $m(\mathcal {R}) = 1$ and $\mathcal {R} = \bigcup _{l=1}^{\infty } \mathcal {R}_l$ is the union of Pesin’s block where $m(\mathcal {R}_l) \rightarrow 1, \mathcal {R}_l \subset \mathcal {R}_{l+1}.$ Moreover, the size of Pesin stable manifolds of points in $\mathcal {R}_l$ is larger than some positive constant $r_l.$ In general, $r_l \rightarrow 0$ when $l \rightarrow \infty .$ We use an absolute continuity result due to Pesin [Reference Barreira and Pesin2, Theorem 4.3.1] which essentially shows the absolute continuity of Pesin’s stable laminations in each block.

Proof of Proposition 3.14

Suppose by contraction that $\mathcal {E}$ is not upper leafwise absolutely continuous. So, there exist a foliated box B and a set $Z\subset B$ with $\mathrm {Vol}_{\mathcal {E}}(Z\cap \mathcal {E}(x))=0$ for m-a.e. $x \in B$ and $m(Z)>0$ . There exists $l \geq 1$ such that $m(Z \cap \mathcal {R}_l)> 0.$ Take a Lebesgue density point $z\in Z\cap \mathcal {R}_l$ such that for V a small neighbourhood of z, we have $m(Z \cap \mathcal {R}_l \cap V)> 0.$

As Pesin stable manifolds are contained in the leaves of $\mathcal {E}$ , our assumption $\mathrm {Vol}_{\mathcal {E}}(Z\cap \mathcal {E}(x))=0$ and upper leafwise absolute continuity of stable manifolds imply that Z has zero measure with respect to conditional measures of m along Pesin stable manifolds in $\mathcal {R}_l$ .) Hence, $m(Z \cap \mathcal {R}_l \cap V) = 0$ , which is a contradiction.

Fix $x\in \mathbb {R}^n$ and denote by $U_r\subset \widetilde {W}^u_A (x)$ the ball of radius r with centre x.

Proposition 3.15. Let $f\colon {\mathbb {T}}^d\rightarrow {\mathbb {T}}^d$ as in Theorem C, then given $\varepsilon>0$ , there is $r_0>0$ and a constant $C_0>0$ such that

for all $n>0$ and $r \geq r_0$ , where $\pi _z$ is the orthogonal projection from $\mathcal {F}(z)$ to $\widetilde {W}_A^u(z)$ (along $\widetilde {E}_A^s$ ) for any $z \in \mathbb {R}^n$ .

Proof of Proposition 3.15

We prove the following claims.

Claim 1. For $z\in {\mathbb {R}}^d$ , the orthogonal projection $\pi _z\colon \mathcal {F}(z)\rightarrow \widetilde {W}^u_A(z)$ is a uniform bi-Lipschitz diffeomorphism.

Proof of Claim 1

By item (2) of Theorem C and continuity of E and F, there is $\alpha>0$ such that the angle $\angle (E,E^u_A)>\alpha $ and $\angle (F, E^s_A)>\alpha .$ So $\widetilde {W}_A^s$ is uniformly transversal to the foliation $\mathcal {F}$ and there is $\beta>0$ such that

(3.5) $$ \begin{align} \|d\pi_z(x)(v)\|\geq\beta\|v\| \end{align} $$

for any $x\in \mathcal {F}(z)$ and $v\in T_x\mathcal {F}(z)$ . This implies that $\mathrm {Jac} \pi _z(x)\neq 0$ . By the inverse function theorem, for each $x\in \mathcal {F}(z)$ , there is a ball $B(x, \delta )\subset \mathcal {F}(z)$ such that $\pi _z|_{B(x, \delta )}$ is a diffeomorphism. In fact, from the proof of the inverse function theorem and equation (3.5), $\delta $ can be taken independent of x. Again, by equation (3.5), there is $\varepsilon>0$ , independent of x such that $B(\pi _z(x), \varepsilon )\subset \pi _z(B(x, \delta ))$ . To prove that $\pi _z$ is surjective, we show that $\pi _z(\mathcal {F}(z))$ is an open and closed subset. As $\pi _z$ is a local homeomorphism, then $\pi _z(\mathcal {F}(z))$ is open. To verify that it is also closed, let $y_n\in \pi _z(\mathcal {F}(z))$ be a sequence converging to y, and hence there is $n_0$ large enough such that $y\in B(\varepsilon ,y_{n_0})$ and, therefore, $y\in {\pi _z}(\mathcal {F}(z))$ . So, $\pi _z$ is surjective. Moreover, $\pi _z$ is a covering map and injectivity follows from the fact that any covering map from a path-connected space to a simply connected space is a homeomorphism.

Let us prove that $\pi _z$ is bi-Lipschitz. In fact,

$$ \begin{align*}\|\pi_z(x)-\pi_z(y)\|\leq\|x-y\|\leq d_{\mathcal{F}}(x,y).\end{align*} $$

Let us show that $\pi _z^{-1}$ is also Lipschitz. This is immediate from equation (3.5). Indeed, let $[x,y]$ be the line segment in $\widetilde {W}^u_A (z)$ connecting x to $y,$ so the set $\pi _z^{-1}([x,y])=\Gamma $ is a smooth curve connecting the points $\pi _z^{-1}(x)$ and $\pi _z^{-1}(y)$ in $\mathcal {F}(z)$ . So,

$$ \begin{align*} d_{\mathcal{F}}(\pi_z^{-1}(x),\pi_z^{-1}(y))\leq \mathrm{length}\,(\Gamma)=\int_{[x,y]}|d\pi_z^{-1}(t)|\,dt\leq \frac{1}{\beta}\|x-y\|.\\[-42pt] \end{align*} $$

Claim 2. Given $\varepsilon>0$ , there is $r_0> 0$ such that $\tilde {f}^n(\pi _x^{-1}(U_r)) \subset \pi _{\tilde {f}^n(x)}^{-1}(U_{r, n})$ for every $r \geq r_0$ and $n \geq 1,$ where $U_{r, n} \subset \widetilde {W}_A^u (\tilde {f}^n(x))$ is a $d_u$ -dimensional ellipsoid with volume bounded above by $(1+\epsilon )^{nd_u} \mathrm {Vol}_{\tilde {W}_A^u}(A^n(U_r)).$

Proof. Let $ r \geq r_0 := ({2R+2K})/{\varepsilon m(A|_{E^u})}$ , where R comes from Proposition 3.11 and $\|\tilde {f}- \tilde {A}\|_{\infty } \leq K.$ We prove that

(3.6) $$ \begin{align} \tilde{f}(\pi_x^{-1}(U_r)) \subset \pi_{\tilde{f}(x)}^{-1}(U_{r, 1}), \end{align} $$

where $U_{r,1} \subset \widetilde {W}^u_A(\tilde {f}(x))$ is obtained from $\tilde {A}(U_r)$ by first applying a homothety of ratio $(1+\epsilon )$ centred at $\tilde {A}(x)$ and then translating by $\tilde {f}(x) - \tilde {A}(x)$ . Observe that $U_{r, 1}$ is an ellipsoid inside the affine $d_u$ dimensional subspace passing through $\tilde {f}(x).$ Take any y on the boundary of $U_r$ . Let $z:=\pi _{\tilde {f}(x)}(\tilde {f}(\pi _x^{-1}(y))) \in \widetilde {W}^u_A(\tilde {f}(x))$ . On the one hand, we have

(3.7) $$ \begin{align} \| z - (\tilde{A}(y) + \tilde{f}(x)- \tilde{A}(x)) \| \leq \| \tilde{f}(x)- \tilde{A}(x) \| + \| z - \tilde{A}(y) \| \leq K + \| z - \tilde{A}(y) \|. \end{align} $$

On the other hand,

(3.8) $$ \begin{align} \| z - \tilde{A}(y) \| &\leq \|z - \tilde{f}(\pi_x^{-1}(y))\| + \| \tilde{f}(\pi_x^{-1}(y))-\tilde{A}(\pi_x^{-1}(y)) \| \nonumber\\ &\quad+ \| \tilde{A}(\pi_x^{-1}(y)) - \tilde{A}(y) \| \nonumber\\ & \leq 2R+K. \end{align} $$

In the above inequalities, we have used Proposition 3.11 two times to get

$$ \begin{align*}\|z - \tilde{f}(\pi_x^{-1}(y)\| \leq R, \end{align*} $$
$$ \begin{align*}\| \tilde{A}(\pi_x^{-1}(y)) - \tilde{A}(y) \| \leq \|y - \pi_x^{-1}(y)\| \leq R, \end{align*} $$

(observe that $y - \pi _x^{-1}(y)$ belongs to the stable subspace of A) and finally

$$ \begin{align*} \| \tilde{f}(\pi_x^{-1}(y)))-\tilde{A}(\pi_x^{-1}(y)) \| \leq \|\tilde{f}-\tilde{A}\|_{\infty} \leq K.\end{align*} $$

Now, putting the inequalities in equations (3.7) and (3.8) together, we get

$$ \begin{align*} \|z - (\tilde{A}(y) + \tilde{f}(x)- \tilde{A}(x))\| \leq 2K + 2R.\end{align*} $$

Observe that $\tilde {A}(y) + \tilde {f}(x)- \tilde {A}(x)$ is the translation of the $\tilde {A}(y)$ and belongs to $\widetilde {W}_A^u(\tilde {f}(x)).$ Indeed, $\tilde {A}(y)- \tilde {A}(x)$ is a vector which belongs to the unstable bundle of $\tilde {A}$ and we identify the unstable bundle at $\tilde {f}(x)$ with the corresponding affine subspace of $\mathbb {R}^n$ passing through $\tilde {f}(x)$ . Now, as the distance between $(1+\epsilon ) \tilde {A}(U_r) $ and $ \tilde {A}(U_r)$ is $ \epsilon r m(\tilde {A}|_{E^u}) \geq 2R + 2K$ (by the choice of r), we conclude that z belongs to the ellipsoid $U_{r, 1} :=(\tilde {f}(x)- \tilde {A}(x)) + (1+\epsilon ) \tilde {A}(U_r)$ which proves equation (3.6). Moreover, observe that $\mathrm {Vol}_{\widetilde {W}^u_A} (U_{r, 1}) =(1+\epsilon )^{d_u} \mathrm {Vol}_{\widetilde {W}^u_A}(\tilde {A}(U_r)) = (1+\epsilon )^{d_u} e^{\sum _{i=1}^{d_u} \unicode{x3bb} ^u_i(A)} \mathrm {Vol}_{\widetilde {W}^u_A} (U_r).$

Figure 1 Volume comparison.

Now we apply again $\tilde {f}$ and obtain

$$ \begin{align*}\tilde{f}^2(\pi_x^{-1}(U_r)) \subset \tilde{f} (\pi_{\tilde{f}(x)}^{-1}(U_{r,1})). \end{align*} $$

As the distance between $\tilde {A}(U_{r, 1})$ and $(1+\epsilon )\tilde {A}(U_{r, 1})$ is larger than $\varepsilon r m(\tilde {A}|_{E^u})$ , similarly as above, we obtain

$$ \begin{align*} \tilde{f} (\pi_{\tilde{f}(x)}^{-1}(U_{r,1})) \subset \pi_{\tilde{f}^2(x)}^{-1}(U_{r, 2}),\end{align*} $$

where $U_{r, 2}$ is a translation of $(1+\varepsilon )^2 \tilde {A}^2(U_r).$ In fact, inductively, we obtain

(3.9) $$ \begin{align} \tilde{f}^{n+1}(\pi_x^{-1}(U_r)) \subset \tilde{f} (\tilde{f}^{n}(\pi_x^{-1}(U_r))) \subset \tilde{f} (\pi_{\tilde{f}^n(x)}^{-1}(U_{r, n})) \subset \pi_{\tilde{f}^{n+1}(x)}^{-1}(U_{r, n+1}), \end{align} $$

where $U_{r, n+1}$ is an ellipsoid with volume less than $(1+\varepsilon )^{(n+1)d_u} e^{(n+1) \sum _{i=1}^{d_u} \unicode{x3bb} ^u_i(A)} \mathrm {Vol}_{\tilde {W}_A^u} (U_r).$ The last inclusion in equation (3.9) follows using the same arguments as above to prove equation (3.6) substituting the ball $U_r$ by the ellipsoid $U_{r, n}.$

By Claim 1, for all $x\in M$ , we have $|\mathrm {Jac}\, \pi ^{-1}_x|$ is uniformly bounded and, consequently, there is a constant $C_0>0$ such that

$$ \begin{align*} \mathrm{Vol}_{\mathcal{F}}(\tilde{f}^n\pi_x^{-1}(U_r))&\leq\mathrm{Vol}_{\mathcal{F}}(\pi_{\tilde{f}^n(x)}^{-1}(U_{r, n}) \leq C_0(1+ \varepsilon)^{nd_u} e^{n \sum_{i = 1}^{d_u} \unicode{x3bb}^u_i(A)}\mathrm{Vol}_{\tilde{W}_A^u}(U_r). \end{align*} $$

It concludes the proof of the Proposition 3.15 (see Figure 1).

Proof of Theorem C

Suppose by contradiction that there is a positive volume set $Z\subset {\mathbb {T}}^d$ such that $\sum _{i=1}^{d_u}\unicode{x3bb} _i^{cu}(f,x)>\sum _{i=1}^{d_u}\unicode{x3bb} _i^u(A)$ for any $x\in Z$ .

Let $P\colon {\mathbb {R}}^d\rightarrow {\mathbb {T}}^d$ be the covering map, $D\subset {\mathbb {R}}^d$ a fundamental domain and ${\widetilde {Z}=P^{-1}(Z)\cap D}$ . We have $\mathrm {Vol}(\widetilde {Z})>0$ .

For each $q\in {\mathbb {N}}\setminus \{0\}$ , we define the set

We have $\bigcup _{q=1}^{\infty }Z_q=\widetilde {Z}$ , and thus there is q such that $m(Z_q)>0$ . For each $x\in Z_q$ , it follows that

So there is $n_0$ such that for $n\geq n_0$ , we have

This implies that

For every $n>0$ , we define

There is $N>0$ with $\mathrm {Vol}(Z_{q,N})>0$ .

For each $x\in D$ , consider $B_x\subset {\mathbb {R}}^d$ a foliated box of $\mathcal {F}.$ By compactness, there is finite cover $\{B_{x_i}\}_{i=1}^{j}$ covering $\overline {D}.$ Since $W^{cu}_f$ is absolutely continuous and the covering map is smooth, then $\mathcal {F}$ is absolutely continuous, and thus there is some i and $p\in B_{x_i}$ such that $\mathrm {Vol}_{\mathcal {F}}(B_{x_i}\cap \mathcal {F}(p)\cap Z_{q,N})>0$ .

There is a set $\pi _p^{-1}(U_r)\subset \mathcal {F}(p)$ , where $\pi _p^{-1}(U_r)$ is as in Proposition 3.15 containing p and r is large enough such that $\mathrm {Vol}_{\mathcal {F}}(\pi _p^{-1}(U_r)\cap Z_{q,N})>0.$ Let $\alpha>0$ be such that $\mathrm {Vol}_{\mathcal {F}}(\pi _p^{-1}(U_r)\cap Z_{q,N})=\alpha \mathrm {Vol}_{\mathcal {F}}(\pi _p^{-1}(U_r)),$ and by Proposition 3.15, we have

(3.10)

However,

(3.11)

Equations (3.10) and (3.11) give us a contradiction when n is large enough, and thus prove Theorem C.

Acknowledgements

J.S.C. was supported by CAPES-PROEX and CNPq process 141224/2013-4. A.T. was supported by the FAPESP thematic project 2017/06463-3 and the CNPq productivity fellowship.

References

Andersson, M., Carrasco, P. D. and Saghin, R.. Non-uniformly hyperbolic endomorphisms. Preprint, 2022, arXiv:2206.08295.Google Scholar
Barreira, L. and Pesin, Y. B.. Lyapunov Exponents and Smooth Ergodic Theory (University Lecture Series, 23). American Mathematical Society, Providence, RI, 2002.Google Scholar
Bochi, J.. Genericity of zero Lyapunov exponents. Ergod. Th. & Dynam. Sys. 22(6) (2002), 16671696.CrossRefGoogle Scholar
Bochi, J., Katok, A. and Rodriguez Hertz, F.. Flexibility of Lyapunov exponents. Ergod. Th. & Dynam. Sys. 42(2) (2022), 554591.CrossRefGoogle Scholar
Bochi, J. and Viana, M.. The Lyapunov exponents of generic volume-preserving and symplectic maps. Ann. of Math. (2) 161 (2005), 14231485.CrossRefGoogle Scholar
Bonatti, C. and Viana, M.. SRB measures for partially hyperbolic systems whose central direction is mostly contracting. Israel J. Math. 115(1) (2000), 157193.CrossRefGoogle Scholar
Brin, M. and Pesin, Y.. Partially hyperbolic dynamical systems. Math. USSR-Izv. 8 (1974), 177218.CrossRefGoogle Scholar
Buzzi, J. and Fisher, T.. Entropic stability beyond partial hyperbolicity. J. Mod. Dyn. 7(4) (2013), 527552.CrossRefGoogle Scholar
Carrasco, P. and Saghin, R.. Extended flexibility of lyapunov exponents for anosov diffeomorphisms. Trans. Amer. Math. Soc. 375 (2022), 34113449.Google Scholar
Costa, J. S. C. and Micena, F.. Pathological center foliation with dimension greater than one. Discrete Contin. Dyn. Syst. 39(2) (2019), 1049.CrossRefGoogle Scholar
Furstenberg, H. and Kesten, H.. Products of random matrices. Ann. Math. Stat. 31(2) (1960), 457469.CrossRefGoogle Scholar
Hammerlindl, A.. Leaf conjugacies on the torus. Ergod. Th. & Dynam. Sys. 33(3) (2013), 896933.CrossRefGoogle Scholar
Hu, H., Hua, Y. and Wu, W.. Unstable entropies and variational principle for partially hyperbolic diffeomorphisms. Adv. Math. 321 (2017), 3168.CrossRefGoogle Scholar
Lyapunov, A. M.. The general problem of the stability of motion. Internat. J. Control 55(3) (1992), 531534.CrossRefGoogle Scholar
Micena, F.. New derived from Anosov diffeomorphisms with pathological center foliation. J. Dynam. Differential Equations 29(3) (2017), 11591172.CrossRefGoogle Scholar
Micena, F. and Tahzibi, A.. Regularity of foliations and Lyapunov exponents of partially hyperbolic dynamics on 3-torus. Nonlinearity 26(4) (2013), 1071.CrossRefGoogle Scholar
Micena, F. and Tahzibi, A.. On the unstable directions and Lyapunov exponents of Anosov endomorphisms. Fund. Math. 235(1) (2016), 3748.Google Scholar
Oseledec, V. I.. A multiplicative ergodic theorem. Lyapunov characteristic numbers for dynamical systems. Trans. Moscow Math. Soc. 19(2) (1968), 197231.Google Scholar
Roldan, M.. Hyperbolic sets and entropy at the homological level. Discrete Contin. Dyn. Syst. 36(6) (2016), 3417.CrossRefGoogle Scholar
Saghin, R.. Volume growth and entropy for ${C}^1$ partially hyperbolic diffeomorphisms. Discrete Contin. Dyn. Syst. 34(9) (2014), 37983801.CrossRefGoogle Scholar
Saghin, R., Valenzuela-Henríquez, P. and Vásquez, C. H.. Regularity of Lyapunov exponents for diffeomorphisms with dominated splitting. Preprint, 2020, arXiv:2002.08459.Google Scholar
Saghin, R. and Xia, Z.. Geometric expansion, Lyapunov exponents and foliations. Ann. Inst. H. Poincaré Anal. Non Linéaire 26 (2009), 689704.CrossRefGoogle Scholar
Tahzibi, A.. Stably ergodic diffeomorphisms which are not partially hyperbolic. Israel J. Math. 142(1) (2004), 315344.CrossRefGoogle Scholar
Figure 0

Figure 1 Volume comparison.