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Symbolic dynamics for pointwise hyperbolic systems on open regions

Published online by Cambridge University Press:  10 September 2024

CHUPENG WU
Affiliation:
College of Mathematics and Statistics, Chongqing University, Chongqing 401331, China (e-mail: 20200601008@cqu.edu.cn)
YUNHUA ZHOU*
Affiliation:
College of Mathematics and Statistics, Chongqing University, Chongqing 401331, China (e-mail: 20200601008@cqu.edu.cn)
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Abstract

Under certain conditions, we construct a countable Markov partition for pointwise hyperbolic diffeomorphism $f:M\rightarrow M$ on an open invariant subset $O\subset M$, which allows the Lyapunov exponents to be zero. From this partition, we define a symbolic extension that is finite-to-one and onto a subset of O that carries the same finite f-invariant measures as O. Our method relies upon shadowing theory of a recurrent-pointwise-pseudo-orbit that we introduce. As a canonical application, we estimate the number of closed orbits for f.

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

1. Introduction

In this paper, we consider a family of systems which is called pointwise hyperbolic, introduced by Chen, Hu, and Zhou in [Reference Chen, Hu and Zhou10], and we construct countable Markov partition with a finite-to-one almost everywhere induced coding for it. A pointwise hyperbolic diffeomorphism $f:M\rightarrow M$ is different from the uniformly hyperbolic situation since the expansion and contraction depend on points. If the system is defined on an open invariant subset $O\subset M$ , as stated in [Reference Chen, Hu and Zhou10], hyperbolicity may not be uniform near the boundary of O. Under some additional conditions (see [Reference Chen, Hu and Zhou10, Assumptions U and S]), the authors proved that such a system has unstable and stable manifolds over any orbit with initial value $x\in O$ . As applications, they give two examples, the almost Anosov diffeomorphisms [Reference Hu and Young15] and gentle perturbations of Katok’s map [Reference Katok17], and show that under certain conditions, the requirements given in Assumptions U and S can be verified. For more details, see [Reference Chen, Hu and Zhou10].

In 2013, Sarig constructed countable Markov partitions with full topological entropy for $C^{1+\alpha } (0<\alpha <1)$ closed surface diffeomorphisms [Reference Sarig22]. His method has been proven to be successful for other classes of systems. Here are some of the recent developments: surface maps with singularities [Reference Lima and Matheus20], $C^{1+\alpha }$ closed manifolds diffeomorphisms in dimension $d\geq 2$ [Reference Ben Ovadia6], non-invertible and/or singular maps [Reference Araujo, Lima and Poletti4, Reference Lima18], and injective semi-conjugacies [Reference Buzzi9]. A comprehensive survey on the construction of Markov partitions for non-uniformly hyperbolic systems can be found in [Reference Lima19].

As pointed out in [Reference Ben Ovadia7], the key engine that allows Sarig’s methods to be applied to more suitable adaptations and generalizations is the Pesin theory. For a fixed constant $\chi>0$ and a non-uniformly hyperbolic orbit, Pesin’s idea [Reference Barreira and Pesin5] was to construct local charts to represent the action of the differential as a small perturbation of a hyperbolic matrix. After the local change of coordinates, although the domain of the chart is no longer uniform in size, as it is in the uniformly hyperbolic situation, this approach produces uniform estimates in charts, that is, one contracts in rate at most $e^{-\chi }$ , and one expands at least $e^{\chi }$ . Thanks to these uniform estimates in charts, one can carry out Pesin’s unstable and stable manifold theorem over a chain (no longer than an orbit), which is then used in Sarig’s and subsequent work mentioned above to construct a coding for big classes of systems.

Unfortunately, similar to 0-summable points considered in [Reference Ben Ovadia7, Definition 2.1], the orbits in pointwise hyperbolic systems may not be the $\chi $ -hyperbolic ones mentioned above since hyperbolicity may become weak near $\partial O$ . An extreme case is an almost Anosov diffeomorphism on the two-dimensional torus studied in [Reference Hu13, Reference Hu and Young15], where the orbit spends almost all the time near the boundary of O for almost every initial point in the sense of Lebesgue measure. Therefore, the estimates in charts may not be held uniform over an orbit. To construct unstable manifolds, in [Reference Chen, Hu and Zhou10], they require a prior condition that the expansion of the map along unstable directions is stronger than the rates of the point moving away from the boundary [Reference Chen, Hu and Zhou10, Assumption U(ii)].

Since a chain or a pseudo-orbit is an orbit up to small errors at each iteration, a slightly stronger assumption (see Assumption US(ii) and (iii) in §2) than [Reference Chen, Hu and Zhou10, Assumptions U(ii) and S(ii)] is indeed necessary if we construct unstable manifolds over the recurrent-pointwise-pseudo-orbit we introduce in Definition 5.1 of §5. However, Assumption US(i) is weaker than [Reference Chen, Hu and Zhou10, Assumptions U(i) and S(i)] since they constructed unstable manifolds along the orbit of f and thus they required the assumption of pointwise dominated splitting. At the same time, the Assumption US(ii) and (iii) we require in this paper were designed to be sufficiently lax that allows us to cover the examples considered in [Reference Chen, Hu and Zhou10].

The paper is organized as follows. In §2, we give definitions and statements of the main results. The results apply to counting the number of closed orbits for pointwise hyperbolic diffeomorphism f under certain pointwise hyperbolic conditions (Assumption US) and regularity assumption (Assumption R). In §3, we represent the dynamics as a small perturbation of a pointwise hyperbolic block-form matrix in a suitable (varying) size of a neighborhood in tangent space (rather than Euclidean space as was done in [Reference Sarig22]) and estimate some inequalities for the ratio of two adjacent neighborhoods under the action of f. Since the charts no longer have uniform estimates (the orbits may have $0$ Lyapunov exponents), we need to find a suitable definition for admissible manifolds on which the graph transform is operable over some suitable edge, this is the content of §4. Section 5 is devoted to the construction of local unstable and stable manifolds over the recurrent-pointwise-pseudo-orbits, which are the limit points of compositions of a graph transform acting on admissible manifolds. Finally, in §6, we show how to employ the shadowing theory of a recurrent-pointwise-pseudo-orbit to construct a Markov partition which induces a finite-to-one almost everywhere coding for pointwise hyperbolic systems on open regions O satisfying Assumptions US and R.

Although our coding works on some examples, the question of whether or not there is an example to clarify the results of the present paper are not included in the work of [Reference Ben Ovadia7], which is an interesting and unresolved question so far. In [Reference Ben Ovadia7, Theorem 8.3 and Corollary 8.4], Ben Ovadia shows that if an almost Anosov diffeomorphisms defined in a two-dimensional torus is topologically transitive and the contraction rates along the stable direction are smaller than 1 even at indifferent fixed point p, then it is 0-summable for every $x\neq p$ , and moreover it is codable. Note that the example of almost Anosov diffeomorphisms in this paper is not necessarily topologically transitive and the contraction rates can reach 1 at p. However, this does not mean that our example includes the former, because near p, the rates in the expansion direction are not limited in [Reference Ben Ovadia7, Definition 8.2(3)], but we require the rates of expansion to be greater than the distance from the point to p (see Assumption US(ii)). We mention that there are non-uniformly contracting maps satisfying Assumption US(iii) in a subset of an open invariant set with every point near p that is not summable. For details, see Example 2.1 in §2.

2. Definition and statements of results

Let M be a $C^{\infty }$ connected compact Riemannian manifold with dimension $d\geq 2$ , and $O \subset~M$ an open connected subset of M. We will always assume that the diameter of M is smaller than one (just multiply the metric by a small constant).

Let $f: M \rightarrow M$ be a $C^{1+\alpha }$ diffeomorphism ( $\alpha>0$ ) such that $f(O)=O$ . Denote by $\|D_{x} f\|$ and $m(D_{x} f)$ the norm and the minimal norm of $D_{x} f$ , respectively. Note that we have $m(D_{x} f)=\|D_{f(x)} f^{-1}\|^{-1}$ .

Definition 2.1. The $C^{1+\alpha }$ diffeomorphism ( $\alpha>0$ ) f is called a pointwise hyperbolic on an invariant set $O \subset M$ if there exist two continuous functions $\unicode{x3bb} ^{u}, \unicode{x3bb} ^{s}: O \rightarrow \mathbb {R}_{+}$ with $\unicode{x3bb} ^{s}(x)<1<\unicode{x3bb} ^{u}(x)$ for any $x\in O$ , and an invariant decomposition $T_{O} M=E^{u} \oplus E^{s}$ such that for any $x \in O$ ,

$$ \begin{align*} \begin{aligned} &\unicode{x3bb}^{u}(x) \leqslant m(D_{x} f|_{E^{u}(x)}), \\ &\|D_{x} f|_{E^{s}(x)}\| \leqslant \unicode{x3bb}^{s}(x), \end{aligned} \end{align*} $$

where $E_{x}^{u}$ and $E_{x}^{s}$ are called unstable and stable subspaces, respectively.

Remark 2.1. Although it is possible that $m(D_{x} f|_{E^{u}(x)}) \rightarrow 1$ or $\|D_{x} f|_{E^{s}(x)}\| \rightarrow 1$ as $x \rightarrow \partial O$ , hyperbolicity is uniform when restricted to any compact set contained in O because of continuity of $\unicode{x3bb} ^{u}(x)$ and $\unicode{x3bb} ^{s}(x)$ .

The following Assumption US is motivated by [Reference Chen, Hu and Zhou10, Assumptions U and S].

Assumption US.

  1. (i) The distributions $E^{u}$ and $E^{s}$ are continuous.

  2. (ii) (U-boundary control) There exist $r_0^u, \beta ^u>0, \gamma ^u>{\max } \{1, \beta ^u / \alpha \}$ , $0<\kappa ^u<1$ , and $C^u>1$ such that for any $x \in O$ satisfying $d(x, \partial O) \leqslant r_0^u$ , we have

    $$ \begin{align*} m(D f|_{E^{u}(x)})^{\kappa^u}-1 \geqslant C^u {\max} \bigg\{d(x, \partial O)^{\beta^u},\bigg(\frac{d(f(x), \partial O)}{d(x, \partial O)}\bigg)^{\gamma^u}-1\bigg\}.\end{align*} $$
  3. (iii) (S-boundary control) There exist $r^s_0, \beta ^s>0, \gamma ^s>{\max } \{1, \beta ^s / \alpha \}$ , $0<\kappa ^s<1$ , and $C^s>1$ such that for any $x \in O$ satisfying $d(x, \partial O) \leqslant r^s_0$ , we have

    $$ \begin{align*} m(D f^{-1}|_{E^{s}(x)})^{\kappa^s}-1 \geqslant C^s {\max} \bigg\{d(x, \partial O)^{\beta^s},\bigg(\frac{d(f^{-1}(x), \partial O)}{d(x, \partial O)}\bigg)^{\gamma^s}-1\bigg\}. \end{align*} $$

Remark 2.2. Assumption US(i) is a corollary of [Reference Chen, Hu and Zhou10, Assumption U(i)], see [Reference Chen, Hu and Zhou10, Lemma 3.1]. It is therefore weaker than the latter.

Remark 2.3. Near the boundary, the forward images of u-admissible manifolds defined in Definition 4.2 grow essentially $m(D_{x} f|_{E^{u}(x)})\rightarrow 1$ as $x \rightarrow \partial O$ , that is, the hyperbolicity may become weak. A priori, the ratio of size of u-admissible manifolds $({d(f(x), \partial O)}/{d(x, \partial O)})^{\gamma ^u}$ may be bigger and far from 1. Fortunately, this is not the case in our setting: Assumption US(ii) means that near the boundary, the expansion rates along the unstable direction are stronger than the ratio of size along the orbit which is near the boundary. Therefore, Assumption US(ii) is required for the unstable manifold theorem (Proposition 5.2(1)) since the size of local unstable manifolds can be recovered under the forward iteration of f when orbits are near the boundary of O.

Assumption US is similar to the boundary condition control in [Reference Chen, Hu and Zhou10, Assumptions U and S]. The additional requirements of $\kappa ^u$ and $\kappa ^s$ were designed to recover the local unstable and stable manifolds, but also sufficiently lax that allow us to cover the examples considered in [Reference Chen, Hu and Zhou10]. It is needed since the local unstable and stable manifold in this paper are constructed over the recurrent-pointwise-pseudo-orbit defined in Definition 5.1 rather than an orbit of f as done in [Reference Chen, Hu and Zhou10]. In fact, under certain conditions (see [Reference Chen, Hu and Zhou10, Assumptions A and K]), for the almost Anosov diffeomorphisms and gentle perturbations of Katok’s map, we can take $({n+2\delta })/({n+3\delta })<\kappa ^t<1$ and $({2\alpha +1})/({2\alpha +1.5})<\kappa ^t<1$ , respectively, where $t=u,s$ . For more details, see [Reference Chen, Hu and Zhou10, Theorems D and E].

Given $a,b>0$ , we write $a\wedge b:=\min \{a,b\}$ , $a\vee b:={\max }\{a,b\}$ . The next assumption is on the regularity of f.

Assumption R. $\alpha>({\beta }/{\gamma }) $ , where $\gamma =\gamma ^u\wedge \gamma ^s$ , $\beta =\beta ^u\vee \beta ^s$ .

Remark 2.4. This is stronger than $\gamma ^u>{\max } \{1, \beta ^u / \alpha \}$ together with $\gamma ^s>{\max } \{1, \beta ^s / \alpha \}$ given in Assumption US(ii) and (iii). However, at the end of the proof of [Reference Chen, Hu and Zhou10, Theorems D and E], we can see that for almost Anosov diffeomorphisms and Katok’s map with gentle perturbations, the authors took $\alpha =n\geq 2, \beta ^u=n+\delta , \gamma ^u=n+2\delta $ where $\delta \in (0,1/3)$ and $\alpha \geq 2, \beta ^u=2\alpha +1/2, \gamma ^u=2\alpha +1$ , respectively. Because of symmetry between the expression of the mapping and its inverse, we can take $\beta ^s=\beta ^u, \gamma ^s=\gamma ^u$ . Therefore, ${\alpha \geq 2}$ selected in [Reference Chen, Hu and Zhou10, Theorems D and E] is enough for Assumption R.

We now give a non-uniformly contracting map satisfying Assumption US(iii) in a subset of O which is unsummable in the sense of [Reference Ben Ovadia7, Definition 2.1]: a point $x \in M$ is called summable if its tangent space decomposes uniquely into $T_x M=H^s(x) \oplus H^u(x)$ where $\text {for all } \xi ^s \in H^s(x), \xi ^u \in H^u(x)$ ,

$$ \begin{align*} \sum_{m \geq 0}\|D_x f^m \xi^s\|^2<\infty, \sum_{m \geq 0}\|D_x f^{-m} \xi^u\|^2<\infty. \end{align*} $$

We mention that contrary to the present work, the distribution $H^s(x) \oplus H^u(x)$ is usually not more than just measurable.

Example 2.1. For simplicity, let us consider a $C^{1+\alpha } (\alpha =2k, k\in \mathbb {N}_+)$ diffeomorphism f of a two-dimensional closed (compact without boundary) connected smooth Riemannian manifold M that has a fixed point p. Suppose f is a non-uniformly contracting map on $O=M/{p}$ and that there exist a neighborhood U of p and a local coordinate system $(x, y)$ with $p = (0, 0)$ . We assume further that on U, f has the form

$$ \begin{align*}f(x,y)=(x-x^{\alpha+1},y-\varepsilon_1yx^\alpha),\end{align*} $$

where $\varepsilon _1>0$ .

Denote $z=(x,y)$ . From

$$ \begin{align*} D_z f=\left(\begin{array}{@{}ll@{}} 1-(1+\alpha)x^\alpha & 0 \\ -\varepsilon_1\alpha yx^{\alpha-1} & 1-\varepsilon_1x^\alpha \end{array}\right)\!, \end{align*} $$

it is easy to verify that if $z\in U$ , we have

$$ \begin{align*} \begin{aligned} D_{z} f^{-1}&=\left(\begin{array}{@{}ll@{}} 1+(1+\alpha)x^\alpha+O(x^{\alpha+1}) & 0\\ \varepsilon_1\alpha yx^{\alpha-1}+yO(x^{2\alpha-1}) & 1+\varepsilon_1x^\alpha+O(x^{\alpha+1}) \end{array}\right)\!. \end{aligned} \end{align*} $$

Now let us consider a subset of U:

$$ \begin{align*} U_1:=U\cap\{z\in U:|y|\leq|x|^{\varepsilon_2}\ \text{where}\ \varepsilon_2>1\}. \end{align*} $$

Claim 1. If $\varepsilon _1>1$ , then there exist $r^s_0, \beta ^s>0, \gamma ^s>{\max } \{1, \beta ^s / \alpha \}$ , $0<\kappa ^s<1$ , and $C^s>1$ such that for any $z \in U_1$ satisfying $\|z\| \leqslant r^s_0$ , we have

$$ \begin{align*} m(D_zf^{-1})^{\kappa^s}-1 \geqslant C^s {\max} \bigg\{\|z\|^{\beta^s},\bigg(\frac{\|f^{-1}(z)\|}{\|z\|}\bigg)^{\gamma^s}-1\bigg\}. \end{align*} $$

Proof of Claim 1

Note that if $z \in U_1$ , we get

$$ \begin{align*} \begin{aligned} D_{z} f^{-1}&=\left(\begin{array}{@{}ll@{}} 1+(1+\alpha)x^\alpha+O(x^{\alpha+1}) & 0\\ O(|x|^{\alpha+\varepsilon_2-1}) & 1+\varepsilon_1x^\alpha+O(x^{\alpha+1}) \end{array}\right)\!, \end{aligned} \end{align*} $$

and thus $m(D_zf^{-1})^{\kappa ^s}-1=\varepsilon _1\kappa ^sx^\alpha +O(|x|^{\alpha +2(\varepsilon _2-1)})$ .

It is easy to see that

$$ \begin{align*} f^{-1}(z)=(x+x^{\alpha+1}+O(x^{\alpha+2}),y+\varepsilon_1yx^\alpha+O(\|z\|^{\alpha+2})). \end{align*} $$

One can choose $r^s_0$ small enough such that $f^{-1}(z)\in U$ for any $z \in U_1$ satisfying $\|z\| \leqslant r^s_0$ , and therefore

$$ \begin{align*} f^{-1}(z)=(x+x^{\alpha+1}+O(x^{\alpha+2}),y+O(|x|^{\alpha+\min\{\varepsilon_2,2\}})). \end{align*} $$

Let us compute

$$ \begin{align*} \begin{aligned} C^s\bigg[\bigg(\frac{\|f^{-1}(z)\|}{\|z\|}\bigg)^{\gamma^s}-1\bigg]&=C^s\bigg[\bigg(\frac{\|f^{-1}(z)\|}{\|z\|}\bigg)^{\gamma^s}-1\bigg]\notag\\ &=C^s\bigg[\bigg(\frac{x^2+2x^{2+\alpha}+y^2+O(|x|^{\alpha+\min\{2\varepsilon_2,3\}})}{x^2+y^2}\bigg)^{\gamma^s/2}-1\bigg]\notag\\ &=C^s\gamma^s\frac{2x^{2+\alpha}+O(|x|^{\alpha+\min\{2\varepsilon_2,3\}})}{2(x^2+y^2)}\notag\\ &\leq C^s\gamma^sx^{\alpha}+O(|x|^{\alpha+\min\{2\varepsilon_2-2,1\}}). \end{aligned} \end{align*} $$

Hence, we get

$$ \begin{align*} m(D_zf^{-1})^{\kappa^s}-1 \geqslant C^s {\max} \bigg\{\|z\|^{\beta^s},\bigg(\frac{\|f^{-1}(z)\|}{\|z\|}\bigg)^{\gamma^s}-1\bigg\}, \end{align*} $$

where $1/\sqrt {\varepsilon _1}<\kappa ^s<1$ , $1<C^s=\gamma ^s<\sqrt [4]{\varepsilon _1}$ , and $\alpha <\beta ^s<\alpha \gamma ^s$ .

Claim 2. If $\varepsilon _1<({\alpha }/{2})+1$ , then $\sum _{m \geq 0}\|D_z f^m({\partial }/{\partial y})\|^2=\infty $ for all $z\in U$ , where $({\partial }/{\partial y})=(0,1)^T$ .

Proof of Claim 2

Denote $z_m=(x_m,y_m):=f^m(z)$ . Notice that $z_m\in U$ for all $z\in U$ . By using induction, we get for all $m\geq 1$ that

$$ \begin{align*} D_z f^m\frac{\partial}{\partial y}=(0,g(x_{m-1})x_m)^T, \end{align*} $$

where $g(x_m)=(({1-\varepsilon _1x^\alpha _m})/({1-x^\alpha _m}))g(x_{m-1})$ and $g(x)=({1-\varepsilon _1x^\alpha })/({x-x^{\alpha +1}})$ .

Clearly, $x_{m-1}=x_{m}+x^{\alpha +1}_{m}+O(x^{\alpha +1}_{m})$ for all $m\geq 1$ since $z_m\in U$ for all $z\in U$ , so by [Reference Hu and Vaienti14, Lemma 3.1], for all large m, we have

$$ \begin{align*} |x_m|=\bigg(\frac{1}{\alpha(m+k)}\bigg)^{1/\alpha}+O\bigg(\frac{1}{m^{\theta}}\bigg) \end{align*} $$

for some integer k, where $\theta>1/\alpha $ .

Now it is easy to get

$$ \begin{align*} \begin{aligned} &\lim_{m\rightarrow\infty}m\bigg(\frac{\|D_z f^m({\partial}/{\partial y})\|^2}{\|D_z f^{m+1}({\partial}/{\partial y})\|^2}-1\bigg)\notag\\ &\quad=\lim_{m\rightarrow\infty}m\bigg(\frac{g(x_{m-1})^2x_m^2}{g(x_m)^2x_{m+1}^2}-1\bigg)\notag\\ &\quad=\frac{2(\varepsilon_1-1)}{\alpha}\notag\\ &\quad<1. \end{aligned} \end{align*} $$

Therefore, $\sum _{m \geq 0}\|D_z f^m({\partial }/{\partial y})\|^2=\infty $ from Raabe’s test. This concludes Claim 2.

In §6, we show how Assumptions US and R for pointwise hyperbolic diffeomorphism f on O are sufficient for the construction of a Markov partition. The conclusion is the existence of a symbolic model for f. Let us give the definitions in the general situation.

Let $\widehat {\mathscr {G}}=(\widehat {V}, \widehat {E})$ be a directed graph with a countable collection of vertices $\widehat {V}$ such that every vertex has at least one edge coming in and at least one edge coming out, that is, for each $v\in \widehat {V}$ , there are $u,w\in \widehat {V}$ and a path $u\rightarrow v\rightarrow w$ which is made up of two edges. The topological Markov shift (TMS) associated to $\widehat {\mathscr {G}}$ is the pair $(\widehat {\Sigma },\widehat {\sigma })$ which is the set

$$ \begin{align*} \widehat{\Sigma}=\{\{v_{n}\}_{n \in \mathbb{Z}} \in \widehat{V}^{\mathbb{Z}}: v_{n} \rightarrow v_{n+1} \text{ for all } n \in \mathbb{Z}\} \end{align*} $$

equipped with the left-shift $\widehat {\sigma }: \widehat {\Sigma } \rightarrow \widehat {\Sigma }$ , $\widehat {\sigma }(\{v_{n}\}_{n \in \mathbb {Z}})=\{v_{n+1}\}_{n \in \mathbb {Z}}$ . An element of $\widehat {\Sigma }$ is denoted by $\underline {v}=\{v_{n}\}_{n \in \mathbb {Z}}$ for the sake of simplicity. We endow $\widehat {\Sigma }$ with the distance $d(\underline {v}, \underline {w}):=\exp [-\min \{|n|: n \in \mathbb {Z}$ such that $v_{n} \neq w_{n}\}]$ . With this metric, $\widehat {\Sigma }$ is a complete separable metric space. Recall that $\widehat {\Sigma }$ is compact if and only if $\widehat {\mathscr {G}}$ is finite. Additionally, $\widehat {\Sigma }$ is locally compact if and only if every vertex of $\widehat {\mathscr {G}}$ has finite ingoing and outgoing degree.

Let $\widehat {\Sigma }^{\#}$ be the recurrent set of $\widehat {\Sigma }$ which is due to Sarig [Reference Sarig22]:

$$ \begin{align*} \widehat{\Sigma}^{\#}:=\{\underline{v}\in\widehat{\Sigma}:&\text{ there exists } u,w\in \widehat{V},\text{ there exists } n_k,m_k\uparrow\infty\\ & \text{ such that}\ v_{n_k}=u\ \text{and}\ v_{-m_k}=w \text{ for all } k\in \mathbb{Z}\}. \end{align*} $$

By the Poincaré recurrence theorem, every $\widehat {\sigma }$ -invariant probability measure is carried by $\widehat {\Sigma }^{\#}$ . Furthermore, every periodic point of $\widehat {\sigma }$ is in $\widehat {\Sigma }^{\#}$ . Notice that when V is finite, $\widehat {\Sigma }^{\#}=\widehat {\Sigma }$ .

Let $\widehat {M}$ be a Riemannian manifold and $\widehat {f}: \widehat {M} \rightarrow \widehat {M}$ be a diffeomorphism.

Definition 2.2. A symbolic model for $\widehat {f}$ is a triple $(\widehat {\Sigma }^{\#}, \widehat {\sigma }, \widehat {\pi })$ satisfying:

  1. (1) $(\widehat {\Sigma }^{\#}, \widehat {\sigma })$ is a recurrent TMS;

  2. (2) $\widehat {\pi }: \widehat {\Sigma }^{\#} \rightarrow \widehat {\pi }(\widehat {\Sigma }^{\#})\subset \widehat {M}$ is continuous and finite-to-one;

  3. (3) $\widehat {\pi } \circ \widehat {\sigma }=\widehat {f} \circ \widehat {\pi }$ on $\widehat {\Sigma }^{\#}$ .

In contrast to the notion of a symbolic model of uniform and non-uniform hyperbolic systems, which requires the map $\widehat {\pi }$ to define in the whole of $\widehat {\Sigma }$ , the notion here assumes not necessarily in $\widehat {\Sigma }$ , but in a recurrent subset $\widehat {\Sigma }^{\#}$ . Intuitively, a diffeomorphism can have many symbolic models. Roughly speaking, an acceptable symbolic model is one for which $\widehat {\pi }(\widehat {\Sigma }^{\#})$ (rather than $\widehat {\pi }(\widehat {\Sigma })$ ) contains a subset where $\widehat {f}$ displays chaotic dynamics. For us, this occurs when $\widehat {f}=f$ is pointwise hyperbolic on an open invariant subset $O\subset M$ satisfying Assumptions US and R.

We assume the metric on M is taken in such a way that for any $x\in O$ , $E^u(x)$ and $E^s(x)$ are pairwise orthogonal [Reference Chen, Hu and Zhou10].

Theorem 2.1. Let f be a pointwise hyperbolic diffeomorphism on an invariant set $O \subset M$ , and suppose it satisfies Assumptions US and R, then f possesses a symbolic model $(\widehat {\Sigma }^{\#}, \widehat {\sigma }, \widehat {\pi })$ . More precisely, there is a set $O^{\#}\subset O$ , a locally compact countable topological Markov shift $(\widehat {\Sigma }, \widehat {\sigma })$ , and a continuous map $\widehat {\pi }:\widehat {\Sigma }^{\#}\rightarrow O $ such that:

  1. (1) $\widehat {\pi } \circ \widehat {\sigma }|_{\widehat {\Sigma }^{\#}}=f \circ \widehat {\pi }$ ;

  2. (2) $\mu (O^{\#})=\mu (O)$ for every finite f-invariant measure $\mu $ ;

  3. (3) $\widehat {\pi }: \widehat {\Sigma }^{\#}\rightarrow O^{\#}$ is a finite-to-one surjective map.

In fact, the subset $O^{\#}\subset O$ in Theorem 2.1 is given by

(2.1) $$ \begin{align} O^{\#}:=\Big\{x\in O: \limsup_{n\rightarrow\infty}d(f^n(x),\partial O)>0\ \text{and}\ \limsup_{n\rightarrow-\infty}d(f^n(x),\partial O)>0\Big\}. \end{align} $$

By the Poincaré recurrence theorem, if $\mu $ is an f-invariant probability measure supported on O, then it is supported on $O^{\#}$ .

We stress the argument in the proof of Theorem 2.1(3) providing more details on the number of the $\widehat {\pi }$ -pre-image, and traditionally refer to the following theorem which precisely characterizes the loss of injectivity of $\widehat {\pi }$ .

Theorem 2.2. For $(\widehat {\Sigma }^{\#}, \widehat {\sigma }, \widehat {\pi })$ given by Theorem 2.1, denote the set of vertices of $\widehat {\Sigma }$ by $\widehat {V}$ . Then there exists a function $N:\widehat {V}\rightarrow \mathbb {N}$ such that for every $x\in O^{\#}$ which can be written as $x=\widehat {\pi }(\underline {v})$ with $v_n=u$ for infinitely many $n>0$ , and $v_n=w$ for infinitely many $n<0$ , we have

$$ \begin{align*} |\widehat{\pi}^{-1}(x)|\leq N(u)N(w). \end{align*} $$

Set $P_n(f):=|\{x\in M:f^n(x)=x\}|$ and let $h_{\mathrm {top}}(f,O):=\sup \{h_{\mathrm {\mathrm {top}}}(f,\mathscr {O}): \mathscr {O}\ \textit {finite} \textit {open cover of } O\}$ denote the topological entropy of $f|_O$ , where the supremum runs over all finite open covers of O. As an application, when $f|_O$ has an ergodic measure of maximal entropy $\mu $ satisfying $h_{\mu }(f|_O)=h_{\mathrm {top}}(f,O)$ , where $h_{\mu }(f|_O)$ is the Kolmogorov–Sinai entropy of $f|_O$ -invariant probability measure $\mu $ , we have the following consequence.

Corollary 2.1. Under the assumptions in Theorem 2.1, suppose that $f|_O$ has an ergodic measure of maximal entropy, then $\text {there exists } C>0$ and $p\in \mathbb {N}$ such that f has at least $Ce^{pnh_{\mathrm {top}}(f,O)}$ periodic points of period $pn$ for all $n\in \mathbb {N}$ , that is,

$$ \begin{align*} P_{pn}(f)\geq Ce^{pnh_{\mathrm{top}}(f, O)}\quad \text{for all } n\in\mathbb{N}. \end{align*} $$

Proof. The proof follows the arguments in [Reference Sarig22, Theorem 1.1], we provide some details.

Write $\widehat {\Sigma }=\widehat {\Sigma }(\widehat {\mathscr {G}})$ and let $\mu $ be an ergodic measure of maximal entropy for $f|_O$ . Proceeding as in [Reference Sarig22, §13], we can lift $\mu $ to an ergodic measure of maximal entropy $\widehat {\mu }$ for $\widehat {\sigma }$ via

(2.2) $$ \begin{align} \widehat{\mu}=\int_{O} \frac{1}{|\widehat{\pi}^{-1}(x)|}\bigg(\sum_{\underline{v} \in \widehat{\pi}^{-1}(x)} \delta_{\underline{v}}\bigg)\, d \mu(x), \end{align} $$

such that $h_{\widehat {\mu }}(\widehat {\sigma })=h_{\mu }(f|_O)$ .

By [Reference Gurevich11, Reference Gurevich12], $\widehat {\mu }$ is supported on a subset $\widehat {\Sigma }(\widehat {\mathscr {G}}^\prime )\subset \widehat {\Sigma }(\widehat {\mathscr {G}})$ , where the smaller TMS $(\widehat {\Sigma }(\widehat {\mathscr {G}}^\prime ),\widehat {\sigma })$ is topologically transitive. For a topologically transitive TMS with countable many vertexes, Gurevič [Reference Gurevich11, Reference Gurevich12] showed a good estimate on $\mathrm {Per}_n(\widehat {\sigma })$ : a topologically transitive TMS $(\widehat {\Sigma }(\widehat {\mathscr {G}}^\prime ),\widehat {\sigma })$ admits at most one measure of maximal entropy $h_{\max }(\widehat {\Sigma }(\widehat {\mathscr {G}}^\prime ))$ , and such a measure exists if and only if $\text {there exists } p\in \mathbb {N}$ such that for every vertex $v\in \widehat {\mathscr {G}}^\prime $ , $\text {there exists } C_v\geq 1$ , such that

$$ \begin{align*} C_v^{-1}\leq\frac{\mathrm{Per}_{pn}(\widehat{\sigma}|_{\widehat{\Sigma}(\widehat{\mathscr{G}}^\prime)},v)}{e^{pnh_{\max}( \widehat{\Sigma}(\widehat{\mathscr{G}}^\prime))}}\leq C_v \end{align*} $$

for all $n\in \mathbb {N}$ , where

$$ \begin{align*} &h_{\max}(\widehat{\Sigma}(\widehat{\mathscr{G}}^\prime)):=h_{\max}(\widehat{\sigma})\\ &\quad={\max}\{h_{\nu}(\widehat{\sigma}): \nu \text{ is } \widehat{\sigma}\text{-invariant Borel probability measure on } \widehat{\Sigma}(\widehat{\mathscr{G}}^\prime)\}, \end{align*} $$

and

$$ \begin{align*} \mathrm{Per}_{pn}(\widehat{\sigma}|_{\widehat{\Sigma}(\widehat{\mathscr{G}}^\prime)},v):=|\{\underline{v}\in\widehat{\Sigma}(\widehat{\mathscr{G}}^\prime): v_0=v, \widehat{\sigma}^{pn}(\underline{v})=\underline{v}\}|. \end{align*} $$

From Theorem 2.1(1) and (3), every periodic point in $\{\underline {v}\in \widehat {\Sigma }(\widehat {\mathscr {G}}^\prime ): v_0=v, \widehat {\sigma }^n(\underline {v})=\underline {v}\}\subset \widehat {\Sigma }^{\#}$ is mapped by $\widehat {\pi }$ to a periodic point of the same period in O. By Theorem 2.2, this mapping is at most $N(v)^2$ -to-one. Therefore, for any $v\in \widehat {\mathscr {G}}^\prime $ and all $n\geq 1$ ,

(2.3) $$ \begin{align} P_{pn}(f)\geq P_{pn}(f|_O)\geq \frac{1}{N(v)^2}\mathrm{Per}_{pn}(\widehat{\sigma}|_{\widehat{\Sigma}(\widehat{\mathscr{G}}^\prime)},v). \end{align} $$

Finally, by assumption and construction, ${h_{\max }(\widehat {\Sigma }(\widehat {\mathscr {G}}^\prime ){\kern-1pt}){\kern-1.2pt}={\kern-1.2pt}h_{\widehat {\mu }}(\widehat {\sigma }){\kern-1.2pt}={\kern-1.2pt}h_{\mu }(f|_O{\kern-1pt}){\kern-1.2pt}={\kern-1.2pt}h_{\mathrm {top}} (f{\kern-1pt},{\kern-1.5pt}O)}$ . Therefore, we have

$$ \begin{align*} P_{pn}(f)\geq \frac{1}{C_vN(v)^2}e^{pnh_{\max}( \widehat{\Sigma}(\widehat{\mathscr{G}}^\prime))}=\frac{1}{C_vN(v)^2}e^{pnh_{\mathrm{top}}(f,O)}.\\[-37pt] \end{align*} $$

Remark 2.5. It should be noted that the reverse of the second inequality in equation (2.3) above might not hold, because $\widehat {\pi }$ may not code trajectories inside $O/O^{\#}$ . A wealth of diffeomorphisms such that the growth rate of $P_{n}(f)$ is superexponential can be found in [Reference Kaloshin16].

Notational convention and standing assumption. From now on, f will be a pointwise hyperbolic on an open invariant subset O of a connected compact smooth Riemannian manifold of dimension greater than 1, and satisfies Assumptions US and R.

Suppose P is a property. The statement ‘for all $\varepsilon $ , small enough P holds’ means ‘ $\text {there exists } \varepsilon _0>0$ which only depends on f, M, $C_{1-4}$ (see Lemma 4.1), and the parameters given by Assumption US(ii) and (iii) such that for all $0<\varepsilon <\varepsilon _0$ , P holds’.

3. Linearization up to small errors

In this section, we will show that $F_{x,y}:=\exp _y^{-1}\circ f\circ \exp _x$ is a small perturbation of a hyperbolic block-form matrix for any $x,y\in O$ such that $F_{x,y}$ is well defined and $d(f(x), y)$ small enough. First, we denote some constants and introduce two main functions, the $\varepsilon (x)$ and $Q(x)$ , which will be used many times throughout the paper.

Denote $r_0=r_0^u\wedge r_0^s$ , where $r_0^u$ and $r_0^s$ are given by Assumption US. Let

(3.1) $$ \begin{align} C_0:=C_0(r_0)=\min_{x\in O(r_0)}\{\min\{m(D f|_{E^{u}(x)}),m(D f^{-1}|_{E^{s}(x)})\}\}, \end{align} $$

here

$$ \begin{align*} O(r_0)=\{x\in O: d(x,\partial O)\geq r_0\} \end{align*} $$

is a compact subset of O since M is compact. Observe that $C_0>1$ as hyperbolicity is uniform in $O(r_0)$ .

Fix a small parameter $\varepsilon>0$ (how small depends on a finite number of inequalities that $\varepsilon $ has to satisfy). For $x\in O$ , set

(3.2) $$ \begin{align} \varepsilon(x)=\varepsilon\min\{r_0^\beta,d(x,\partial O)^\beta\}, \end{align} $$

where $\beta =\beta ^u\vee \beta ^s$ as in Assumption R. We start with a basic lemma.

Lemma 3.1. For all $\varepsilon $ small enough and for every $x\in O$ ,

(3.3) $$ \begin{align} C\varepsilon(x)\leq\min\{m(D f|_{E^{u}(x)})^{\kappa}-1,m(D f^{-1}|_{E^{s}(x)})^{\kappa}-1\}, \end{align} $$

where $C=C^u\wedge C^s$ and $\kappa =\kappa ^u\vee \kappa ^s$ .

Proof. Our first constraint on $\varepsilon $ is that it has to be small so that

$$ \begin{align*} 0<\varepsilon\leq\min \bigg\{\frac{C_0^\kappa-1}{Cr_0^\beta},1 \bigg\}. \end{align*} $$

Recall that the diameter of M is smaller than $1$ . There are the following two cases.

Case 1. $\varepsilon (x)\hspace{-0.5pt}=\hspace{-0.5pt}\varepsilon r_0^\beta $ . In this case, we note that $x\hspace{-1pt}\in\hspace{-1pt} O(r_0)$ and $1\hspace{-1pt}<\hspace{-1pt}C_0\hspace{-1pt}\leq\hspace{-1pt} \min \{m(D f|_{E^{u}(x)}), m(D f^{-1}|_{E^{s}(x)})\}$ . Therefore,

$$ \begin{align*} \begin{aligned} C\varepsilon(x)\leq C_0^\kappa-1\leq\min\{m(D f|_{E^{u}(x)})^{\kappa}-1,m(D f^{-1}|_{E^{s}(x)})^{\kappa}-1\}. \end{aligned} \end{align*} $$

Case 2. $ \varepsilon (x)=\varepsilon d(x,\partial O)^\beta $ . Now we have $d(x,\partial O)\leq r_0$ . Since $\beta =\beta ^u\vee \beta ^s$ , $C=C^u\wedge C^s$ , and $\kappa =\kappa ^u\vee \kappa ^s$ , the required inequality is an immediate result of Assumption US(ii) and (iii).

Now we fix another parameter $0<\delta <\min \{1,\alpha -{\beta }/{\gamma }\}$ , which is well defined from Assumption R. Setting

(3.4) $$ \begin{align} Q(x)=\varepsilon^{{2}/({\alpha-\delta})}\min\{r_0^\gamma,d(x,\partial O)^{\gamma}\}, \end{align} $$

note that $Q(x)^{\alpha -\delta }\leq \varepsilon \varepsilon (x)$ because $(\alpha -\delta )\gamma>\beta $ and $Q(x)\leq d(x,\partial O)$ for $\gamma>1$ when $0<\varepsilon <1$ .

Lemma 3.2. The following holds for all $\varepsilon $ small enough. For every $x\in O$ , we have

(3.5) $$ \begin{align} \frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)}\leq\frac{Q(f(x))}{Q(x)}\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1 \end{align} $$

and

(3.6) $$ \begin{align} C\varepsilon(x)\leq\min\{m(D f|_{E^{u}(x)})^{\kappa}-1,1-\|Df|_{E^s(x)}\|^{\kappa}\}. \end{align} $$

A similar statement holds for $f^{-1}$ .

Proof. We give the proofs for equations (3.5) and (3.6). The proofs for $f^{-1}$ are almost identical, the major change being the substitution of $f^{-1}$ for f.

For the companion inequality in equation (3.5), there are four cases. It is worth pointing out that Case 2 is the most interesting, since it is the case where both x and $f(x)$ are close to $\partial O$ , and hence there is little hyperbolicity.

Case 1. $Q(x)=Q(f(x))=\varepsilon ^{{2}/({\alpha -\delta })}r_0^\gamma $ . In this case, equation (3.5) is straightforward since for any $x\in O$ ,

$$ \begin{align*} \begin{aligned} \frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)}\leq1=\frac{Q(f(x))}{Q(x)}=1\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1. \end{aligned} \end{align*} $$

Case 2. $Q(x)=\varepsilon ^{{2}/({\alpha -\delta })}d(x, \partial O)^\gamma $ and $Q(f(x))=\varepsilon ^{{2}/({\alpha -\delta })}d(f(x), \partial O)^\gamma $ . Equivalently, $d(x, \partial O) \leq r_0\leq r_0^u$ and $d(f(x), \partial O) \leq r_0\leq r_0^s$ . Taking Assumption US(ii) and (iii) into consideration, we find in this case that

$$ \begin{align*} \bigg(\frac{d(f(x), \partial O)}{d(x, \partial O)}\bigg)^{\gamma^u}\leq\frac{1}{C^u}(m(D f|_{E^{u}(x)})^{\kappa^u}-1)+1 \end{align*} $$

and

$$ \begin{align*} \begin{aligned} \bigg(\frac{d(x, \partial O)}{d(f(x), \partial O)}\bigg)^{\gamma^s}&\leq\frac{1}{C^s}(m(D f^{-1}|_{E^{s}(f(x))})^{\kappa^s}-1)+1\notag\\ &=\frac{1}{C^s}(\|Df_{E^{s}(x)}\|^{-\kappa^s}-1)+1, \end{aligned} \end{align*} $$

where in the last equality, we used that $m(D f^{-1}|_{E^{s}(f(x))})^{\kappa ^s}=\|D f|_{E^{s}(x)}\|^{-\kappa ^s}$ .

If $({d(f(x),\partial O)}/{d(x,\partial O)})\geq 1$ , on the one hand,

$$ \begin{align*} \frac{Q(f(x))}{Q(x)}=\bigg(\frac{d(f(x),\partial O)}{d(x,\partial O)}\bigg)^\gamma>1\geq\frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)}. \end{align*} $$

On the other hand, since $\gamma \leq \gamma ^u$ , $C\leq C^u$ , $\kappa ^u\leq \kappa $ , we have

$$ \begin{align*} \begin{aligned} \frac{Q(f(x))}{Q(x)}&=\bigg(\frac{d(f(x),\partial O)}{d(x,\partial O)}\bigg)^\gamma\notag\\ &\leq\bigg(\frac{d(f(x), \partial O)}{d(x, \partial O)}\bigg)^{\gamma^u}\notag\\ &\leq\frac{1}{C^u}(m(D f|_{E^{u}(x)})^{\kappa^u}-1)+1\notag\\ &\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1. \end{aligned} \end{align*} $$

Therefore, the companion inequality in equation (3.5) holds when $({d(f(x),\partial O)}/ {d(x,\partial O)})\geq 1$ in Case 2.

Now if $0<({d(f(x),\partial O)}/{d(x,\partial O)})\leq 1$ , then

$$ \begin{align*} \frac{Q(f(x))}{Q(x)}\leq1\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1. \end{align*} $$

Using $\gamma \leq \gamma ^s$ , $C\leq C^s$ , $\kappa ^s\leq \kappa $ , we obtain

$$ \begin{align*} \begin{aligned} \frac{Q(f(x))}{Q(x)}&=\bigg(\frac{d(f(x),\partial O)}{d(x,\partial O)}\bigg)^\gamma\notag\\ &\geq\bigg(\frac{d(f(x), \partial O)}{d(x, \partial O)}\bigg)^{\gamma^s}\notag\\ &\geq\bigg[\frac{1}{C^s}(\|Df_{E^{s}(x)}\|^{-\kappa^s}-1)+1\bigg]^{-1}\notag\\ &\geq\bigg[\frac{1}{C}(\|Df_{E^{s}(x)}\|^{-\kappa}-1)+1\bigg]^{-1}\notag\\ &=\frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)}. \end{aligned} \end{align*} $$

This completes the proof of equation (3.5) in Case 2.

Case 3. $Q(x)=\varepsilon ^{{2}/({\alpha -\delta })}d(x, \partial O)^\gamma $ and $Q(f(x))=\varepsilon ^{{2}/({\alpha -\delta })}r_0^\gamma $ . Now $d(x, \partial O)^\gamma \leq r_0^\gamma \leq d(f(x), \partial O)^\gamma $ , so it follows that

$$ \begin{align*} \frac{Q(f(x))}{Q(x)}=\frac{r_0^\gamma}{d(x, \partial O)^\gamma}\geq1\geq\frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)}. \end{align*} $$

In this case, since $d(x, \partial O)\leq r_0^u$ and $({d(f(x),\partial O)}/{d(x,\partial O)})\geq 1$ , we have

$$ \begin{align*} \begin{aligned} \frac{Q(f(x))}{Q(x)}&\leq\bigg(\frac{d(f(x),\partial O)}{d(x,\partial O)}\bigg)^\gamma\notag\\ &\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1 \end{aligned} \end{align*} $$

as in Case 2 when $({d(f(x),\partial O)}{d(x,\partial O)})\geq 1$ .

Case 4. $Q(x)=\varepsilon ^{{2}/({\alpha -\delta })}r_0^\gamma $ and $Q(f(x))=\varepsilon ^{{2}/({\alpha -\delta })}d(f(x), \partial O)^\gamma $ . In this case, $d(f(x), \partial O)^\gamma \leq r_0^\gamma \leq d(x, \partial O)^\gamma $ , then

$$ \begin{align*} \frac{Q(f(x))}{Q(x)}=\frac{d(f(x), \partial O)^\gamma}{r_0^\gamma}\leq1\leq\frac{1}{C}(m(D f|_{E^{u}(x)})^{\kappa}-1)+1. \end{align*} $$

Notice that $d(f(x), \partial O)\leq r_0^s$ and $0<({d(f(x),\partial O)}/{d(x,\partial O)})\leq 1$ , so we obtain

$$ \begin{align*} \begin{aligned} \frac{Q(f(x))}{Q(x)}&\geq\bigg(\frac{d(f(x),\partial O)}{d(x,\partial O)}\bigg)^\gamma\notag\\ &\geq\frac{C}{\|Df|_{E^s(x)}\|^{-\kappa}+(C-1)} \end{aligned} \end{align*} $$

as in Case 2 when $0<({d(f(x),\partial O)}/{d(x,\partial O)})\leq 1$ .

Hence, the companion inequality in equation (3.5) is proved. From Lemma 3.1, it remains to show that $C\varepsilon (x)\leq 1-\|Df|_{E^s(x)}\|^{\kappa }$ for small $\varepsilon>0$ such that

$$ \begin{align*} 0<\varepsilon\leq\min\bigg\{1,\frac{C_0^\kappa-1}{Cr_0^\beta},\frac{1-C_0^{-\kappa}}{Cr_0^\beta}, \frac{1}{A_s^\beta(C^f)^{\kappa^s}}\bigg\}, \end{align*} $$

where $A_s:=[({1}/{C^s})((C^f)^{\kappa ^s}-1)+1]^{1/\gamma ^s}>1$ and $C^f:={\max }_{x\in M}\{{\max }\{\|D_xf\|, \|D_x f^{-1}\|\}\}$ .

For any $x\in O$ , $f(x)\in O$ , there are the following two cases.

Case 1. $\varepsilon (f(x))=\varepsilon r_0^\beta $ . In this case, observe that $f(x)\in O(r_0)$ , so using equation (3.1), we get

$$ \begin{align*} C_0\leq m(Df^{-1}|_{E^s(f(x))})=\|Df|_{E^s(x)}\|^{-1}, \end{align*} $$

and hence

$$ \begin{align*} C\varepsilon(x)\leq C\varepsilon r_0^\beta\leq1-C_0^{-\kappa}\leq1-\|Df|_{E^s(x)}\|^{\kappa}. \end{align*} $$

Case 2. $\varepsilon (f(x))=\varepsilon d(f(x),\partial O)^\beta $ . Now $d(f(x),\partial O)\leq r_0^s$ , and from Assumption US(iii), we find

$$ \begin{align*} \bigg(\frac{d(x, \partial O)}{d(f(x), \partial O)}\bigg)^{\beta}\leq A_s^\beta \end{align*} $$

and

$$ \begin{align*} \begin{aligned} C^s d(f(x),\partial O)^{\beta^s}&\leq m(Df^{-1}|_{E^s(f(x))})^{\kappa^s}(1- m(Df^{-1}|_{E^s(f(x))})^{-\kappa^s})\notag\\ &=m(Df^{-1}|_{E^s(f(x))})^{\kappa^s}(1- \|D f|_{E^{s}(x)}\|^{\kappa^s})\notag\\ &\leq(C^f)^{\kappa^s}(1-\|D f|_{E^{s}(x)}\|^{\kappa^s}). \end{aligned} \end{align*} $$

Therefore, we obtain that

$$ \begin{align*} \begin{aligned} C\varepsilon(x)&\leq \varepsilon C d(x,\partial O)^\beta\notag\\ &\leq\varepsilon A_s^\beta C^sd(f(x), \partial O)^\beta\notag\\ &\leq \varepsilon A_s^\beta(C^f)^{\kappa^s} (1-\|D f|_{E^{s}(x)}\|^{\kappa^s})\notag\\ &\leq 1-\|D f|_{E^{s}(x)}\|^{\kappa}. \end{aligned}\\[-35pt] \end{align*} $$

Before we begin, recall the following basic fact from Riemannian geometry: since M is compact, there exist $r(M),\rho (M)>0$ such that for every $z\in M$ , the exponential map $\exp _z$ maps $T_zM(r(M)):=\{v\in T_zM:\|v\|< r(M)\}$ diffeomorphically (that is, $\exp _z$ is a bijective $C^\infty $ map whose $\exp _z^{-1}$ is also $C^\infty $ ) onto a neighborhood of $B(z,\rho (M)):=\{y\in M:d(y,z)< \rho (M)\}$ in a 2-bi-Lipschitz way.

For any $x\in O$ , let $B_x^u(Q(x))$ and $B_x^s(Q(x))$ denote the closed balls of radius $Q(x)$ about the origin in $E^u(x)$ and $E^s(x)$ , respectively. Denote the $Q(x)$ -square centered at x by

(3.7) $$ \begin{align} S_x=B_x^u(Q(x))\oplus B_x^s(Q(x)). \end{align} $$

Fix $\varepsilon>0$ small enough such that $Q(x)<\min \{{r(M)}/{\sqrt {2}},{\rho (M)}/{2\sqrt {2}}\}$ , and $\exp _x$ maps $S_x\hspace{-1pt}\subset\hspace{-1pt} T_xM(r(M))$ diffeomorphically into a subset of $B(x,2\sqrt {2}Q(x))\hspace{-1pt}\subset\hspace{-1pt} B(x,\rho (M))$ . It fol lows that $f\hspace{-0.5pt}\circ\hspace{-0.5pt} \exp _x$ maps $S_x C^{1+\alpha }$ diffeomorphically into a subset of $B(f(x),2\sqrt {2}C^fQ(x))$ . Moreover, if necessary, choosing a smaller $\varepsilon $ such that $Q(x)<({\rho (M)}/{2\sqrt {2}C^f})$ , then for $y\in O$ satisfying $d(f(x),y)<\rho (M)-2\sqrt {2}C^fQ(x)$ , $f\circ \exp _x$ maps $S_x C^{1+\alpha }$ diffeomorphically into $B(f(x),2\sqrt {2}C^fQ(x))\subset B(y,d(y,f(x))+2\sqrt {2}C^fQ(x))$ , which is a subset of $B(y,\rho (M))$ . Since $\exp ^{-1}_y$ is a diffeomorphism on $B(y,\rho (M))$ , the map $F_{x,y}: S_x \rightarrow T_{y}M$ defined by

(3.8) $$ \begin{align} F_{x,y}:=\exp^{-1}_y\circ f\circ \exp_x \end{align} $$

is well defined and a $C^{1+\alpha }$ diffeomorphism onto its image.

For $x\in O$ , denote by $P_x^u$ and $P_x^s$ the projections from $T_xM$ to $E^u(x)$ and $E^s(x)$ , respectively. Whenever $F_{x,y}$ is defined, with respect to $E^u\oplus E^s$ , we have

(3.9) $$ \begin{align} D_0F_{x,y}=\left(\begin{array}{@{}cc@{}} D^{uu}_{x,y} & D^{us}_{x,y} \\ D^{su}_{x,y} & D^{ss}_{x,y} \\ \end{array}\right)\!, \end{align} $$

where $D^{\tau t}_{x,y}=P_y^{\tau }\circ D_{f(x)}\exp ^{-1}_y\circ D_xf|_{E^t(x)}:B_x^t(Q(x))\rightarrow E^\tau (y)$ , $\tau ,t=u,s$ .

We write $F_{x,y}|_{S_x}=D_0F_{x,y}+\phi _{x,y}$ in the form

(3.10) $$ \begin{align} &F_{x,y}(v_x^u,v_x^s)\nonumber\\ &\quad=(D^{uu}_{x,y}(v_x^u)+D^{us}_{x,y}(v_x^s)+\phi^u_{x,y}(v_x^u,v_x^s), D^{ss}_{x,y}(v_x^s)+D^{su}_{x,y}(v_x^u)+\phi^s_{x,y}(v_x^u,v_x^s)) \end{align} $$

under the basis $(E^u,E^s)$ for all $v_x=(v_x^u,v_x^s)\in S_x$ . Note that $\|\phi _{x,y}(0)\|=d(f(x),y)$ and $D_0\phi _{x,y}=0$ .

Since the distribution $E^u$ is continuous under Assumption US(i), for $\varepsilon>0$ small enough and any $x\in O$ , there exists a local monotone function $\delta ^u(\cdot ): (0,\varepsilon (x)]\rightarrow (0, \rho (M)-2\sqrt {2}C^fQ(x))$ in the sense that $\delta ^u(a)\leq \delta ^u(b)$ if $0<a\leq b\leq \varepsilon (x)$ such that for all $y\in B(f(x),\delta ^u(\varepsilon (x)))$ , we have

(3.11) $$ \begin{align} \|D^{u s}_{x,y}\|\leq\varepsilon\varepsilon(x)\quad \text{and}\quad |m(D^{uu}_{x,y})- m(D f|_{E^{u}(x)})| \leq\varepsilon\varepsilon(x). \end{align} $$

Similarly, we have

(3.12) $$ \begin{align} \|D^{s u}_{x,y}\|\leq\varepsilon\varepsilon(x),\quad \text{and}\quad |\|D f|_{E^{s}(x)}\|-\|D^{ss}_{x,y}\|| \leq\varepsilon\varepsilon(x). \end{align} $$

By the same reason, for any $y\in O$ and any $x\in B(f^{-1}(y),\delta ^s(\varepsilon (y))$ , where $\delta ^s(\varepsilon (y))$ is defined analogous to $\delta ^u(\varepsilon (x))$ , by considering $F_{x,y}^{-1}=\exp _{x}^{-1} \circ f^{-1} \circ \exp _y$ instead of $F_{x,y}$ , we can get that $F_{x,y}^{-1}$ is well defined and a $C^{1+\alpha }$ diffeomorphism from $S_y$ onto its image, also to get four similar inequalities like equations (3.11) and (3.12).

Proposition 3.1. The following holds for all $\varepsilon>0$ small enough. For all $x\in O$ , there is a local monotone function $0<\delta ^u(\varepsilon (x))<\varepsilon \varepsilon (x)$ such that for $y\in O$ satisfying $d(f(x),y)<\delta ^u(\varepsilon (x))$ , $F_{x,y}|_{S_x}=D_0F_{x,y}+\phi _{x,y}$ can be put in the form

$$ \begin{align*}&F_{x,y}(v_x^u,v_x^s)\\ &\quad=(D^{uu}_{x,y}(v_x^u)+D^{us}_{x,y}(v_x^s)+\phi^u_{x,y}(v_x^u,v_x^s),D^{ss}_{x,y}(v_x^s)+D^{su}_{x,y}(v_x^u)+\phi^s_{x,y}(v_x^u,v_x^s))\end{align*} $$

under the basis $(E^u,E^s)$ for all $v_x=(v_x^u,v_x^s)\in S_x$ , where $\phi _{x,y}:=(\phi ^u_{x,y},\phi ^s_{x,y})$ satisfies:

  1. (1) $\|\phi _{x,y}(0)\|=d(f(x),y)$ ;

  2. (2) $\|D\phi _{x,y}\|_{C^0}\leq \varepsilon \varepsilon (x)$ ;

  3. (3) $\|D_v\phi _{x,y}-D_w\phi _{x,y}\|\leq \varepsilon \varepsilon (x)\|v-w\|^{\delta /2}$ for all $v,w\in S_x$ .

A similar statement holds for $F_{x,y}^{-1}=\exp _{x}^{-1} \circ f^{-1} \circ \exp _y$ defined on $S_{y}$ for all $x\in B(f^{-1}(y),\delta ^s(\varepsilon (y)))$ .

Proof. Since $F_{x,y}$ is $C^{1+\alpha }$ , there is $ \hat {C}>0$ such that for any $v,w\in S_{x}$ ,

$$ \begin{align*} \|D_vF_{x,y}-D_wF_{x,y}\|\leq \hat{C}\|v-w\|^\alpha. \end{align*} $$

Fix $\varepsilon>0$ small enough so that

$$ \begin{align*} \varepsilon^{{\delta}/({\alpha-\delta})}\leq\min\bigg\{1,\frac{1}{(2\sqrt{2})^{\alpha-{\delta}/{2}}\hat{C}}\bigg\}. \end{align*} $$

Part (1) is free and part (2) is a special case of part (3) when $w=0$ since $D_0\phi _{x,y}=0$ . Then what we need to check is property (3).

In fact, we have

$$ \begin{align*} \begin{aligned} \|D_v\phi_{x,y}-D_w\phi_{x,y}\|&=\|D_vF_{x,y}-D_wF_{x,y}\|\notag\\ &\leq \hat{C}\|v-w\|^{\alpha-{\delta}/{2}}\|v-w\|^{\delta/2}\notag\\ &\leq (2\sqrt{2})^{\alpha-{\delta}/{2}}\hat{C}Q(x)^{\delta/2} Q(x)^{\alpha-\delta}\|v-w\|^{\delta/2}\notag\\ &\leq (2\sqrt{2})^{\alpha-{\delta}/{2}}\hat{C}\varepsilon^{{\delta}/({\alpha-\delta})}\cdot\varepsilon\varepsilon(x)\|v-w\|^{\delta/2}\notag\\ &\leq \varepsilon\varepsilon(x)\|v-w\|^{\delta/2}. \end{aligned} \end{align*} $$

By considering $f^{-1}$ in the charts $\exp _y$ of point y and $\exp _x^{-1}$ of $f^{-1}(y)$ when x is near $f^{-1}(y)$ , we can apply a similar treatment to $F_{x,y}^{-1}$ . The details are left to the reader.

4. Admissible manifolds and graph transform along the edge

In this section, denote $t:= u,s$ . As usual, we give the canonical definition of t-manifolds first.

Definition 4.1. Suppose $x\in O$ .

  1. (1) A u-manifold at x is a manifold $V_x^{u}= \exp _{x}\{(v^u,\sigma _x^u(v^u))\in T_xM:\|v^u\| \leq Q (x)\}\subset M$ , where $\sigma ^u:B_x^u(Q(x)) \rightarrow E^s(x)$ is a $C^{1+\delta /2}$ function such that $\|\sigma _x^u\|_{C^0}\leq Q(x)$ .

  2. (2) Similarly, an s-manifold at x is a manifold $V_x^{s}=\exp _{x}\{(\sigma ^s_x(v^s),v^s):\|v^s\| \leq Q(x)\}$ where $\sigma ^s_x:B_x^s(Q(x)) \rightarrow E^u(x)$ is a $C^{1+\delta /2}$ function such that $\|\sigma _x^s\|_{C^0}\leq Q(x)$ .

Thus, every t-manifold at x is contained in $\exp _{x}(S_x)$ . For any $x\in O$ , we call $\sigma ^t_x$ the representing functions of $V_x^{t}$ .

Among the t-manifolds, we are interested in those that can eventually represent unstable and stable manifolds, and for that, we require some extra conditions on the representing functions. We call them admissible manifolds.

Definition 4.2. For any $x\in O$ , a t-admissible manifold at x is a t-manifold $V_x^{t}$ where the representing function $\sigma ^t_x$ satisfies the following three conditions:

  1. (AM1) $\|\sigma _x^t(0)\| \leq 10^{-3}Q(x)$ ;

  2. (AM2) $\|D\sigma _x^t\|_{C^0} \leq \sqrt {\varepsilon }$ ;

  3. (AM3) $\|D\sigma _x^t\|_{C^{\delta /2}}:=\|D\sigma _x^t\|_{C^{0}}+\operatorname {Hol}_{\delta /2}(D\sigma ^t_x) \leq \tfrac 12$ , with norms taken in $B_x^t(Q(x))$ .

Observe that the upper bound of $\|\sigma _x^t(0)\|$ is linear in $Q(x)$ , while the estimate on the derivative of a representing function is constant in our setting rather than of the order of $Q(x)^{\delta /2}$ as in [Reference Sarig22, Definition 4.8]. This distinction will be clear when we start to establish an estimate in the graph transform along the edge (Definition 4.4).

Let $\mathscr {V}_{x}^t$ be the space of all t-admissible manifolds at $x\in O$ . We introduce two metrics on $\mathscr {V}_{x}^{t}$ as follows: for $V^t_{1}, V^t_{2} \in \mathscr {V}_x^{t}$ with representing functions $\sigma ^t_{1}, \sigma ^t_{2}$ , respectively, put

$$ \begin{align*} d_{C^i}(V^t_{1}, V^t_{2}):=\|\sigma^t_{1}-\sigma^t_{2}\|_{C^{i}},\ i=0,1, \end{align*} $$

where

$$ \begin{align*} \|\sigma^t_{1}-\sigma^t_{2}\|_{C^{0}}&={\max}_{v_x\in B_x^t(Q(x))}\|\sigma^t_{1}(v_x)-\sigma^t_{2}(v_x)\|,\\ \|\sigma^t_{1}-\sigma^t_{2}\|_{C^{1}}&=\|\sigma^t_{1}-\sigma^t_{2}\|_{C^{0}}+\|D\sigma^t_{1}-D\sigma^t_{2}\|_{C^{0}}, \end{align*} $$

and

$$ \begin{align*} \|D\sigma^t_{1}-D\sigma^t_{2}\|_{C^{0}}={\max}_{v_x\in B_x^t(Q(x))}\|D_{v_x}\sigma^t_{1}-D_{v_x}\sigma^t_{2}\|. \end{align*} $$

If $\varepsilon>0$ is small enough, from conditions (AM1) and (AM2), we have $\|\sigma _x^t\|_{C^0}\leq Q(x)$ , because for all $v_x\in B_x^t(Q(x))$ ,

(4.1) $$ \begin{align} \|\sigma_x^t(v_x)\|&\leq\|\sigma_x^t(0)\|+\operatorname{Lip}(\sigma_x^t)\|v_x\| \leq 10^{-3}Q(x)\nonumber\\ &\quad+\sqrt{\varepsilon}\|v_x\| \leq(10^{-3}+\sqrt{\varepsilon})Q(x)<10^{-2}Q(x), \end{align} $$

where in the last inequality, we require $\varepsilon>0$ to be small. In particular, $\sigma _x^u$ maps the ball $B_x^u(10^{-2}Q(x))$ into $B_x^s(10^{-2}Q(x))$ , and maps $B_x^u(Q(x))$ into $B_x^s(Q(x))$ .

Proposition 4.1. For every $x\in O$ , the following holds for $\varepsilon>0$ small enough. For every $V_x^{u} \in \mathscr {V}_x^{u}$ and $V_x^{s} \in \mathscr {V}_x^{s}$ , the following hold:

  1. (1) $V_x^{u}$ and $V_x^{s}$ intersect at a single point $P=P(V_x^{u},V_x^{s}):=\exp _{x}(w)\in O$ , and $\|w\|\leq 50^{-1}Q(x)$ ;

  2. (2) P is a Lipschitz function of $(V_x^u,V_x^s)$ , with Lipschitz constant less than ${2}/({1-\sqrt {\varepsilon }})$ .

Proof. We follow the same strategy of [Reference Sarig22, Proposition 4.11].

(1) To prove the non-emptiness of $V_x^{u}\cap V_x^{s}$ , we fix $V_x^{t}$ with representing function $\sigma _x^t$ . From a pedagogical perspective, the ideas of the proof are very simple. If we suppose the intersections of $V_x^{u}$ and $V_x^{s}$ are non-empty, it corresponds to points $(v^u,v^s)$ that satisfy $\exp _x(v^u,\sigma _x^u(v^u))=\exp _x(\sigma _x^s(v^s),v^s)$ , so it is the solution of the equation:

$$ \begin{align*} \begin{cases} v^u=\sigma_x^s(v^s), \\ v^s=\sigma_x^u(v^u). \end{cases} \end{align*} $$

Hence, the trick of the proof is to find the fixed points of $\sigma _x^s \circ \sigma _x^u$ on $B_x^u(Q(x))$ .

We first note that $\sigma _x^s \circ \sigma _x^u$ maps the ball $B_x^u(10^{-2}Q(x))$ into itself from equation (4.1) if $\varepsilon>0$ is small enough. It follows that $\sigma _x^s \circ \sigma _x^u$ is an $\varepsilon $ -contraction of $B_x^u(10^{-2}Q(x))$ into itself. Indeed, from condition (AM2), we have $\|D(\sigma _x^s\hspace{-0.5pt} \circ\hspace{-0.5pt} \sigma _x^u)\|_{C^0}\hspace{-0.5pt}\leq\hspace{-0.5pt} \|D\sigma _x^s\|_{C^0}\|D\sigma _x^u\|_{C^0}\hspace{-0.5pt}\leq\hspace{-0.5pt} \varepsilon $ . By the Banach fixed point theorem, $\sigma _x^s \circ \sigma _x^u$ has a unique fixed point: $(\sigma _x^s \circ \sigma _x^u)(v_0^u)=v_0^u,$ where $v_0^u\in B_x^u(10^{-2}Q(x))$ .

Let $v_0^s:=\sigma _x^u(v_0^u)$ , $w:=(v_0^u,v_0^s)$ , then $V_x^{u}$ intersects $V_x^{s}$ at $P:=\exp _{x}(w)$ . Indeed, $P \in V_x^{u}$ is evident because $v_0^s=\sigma _x^u(v_0^u)$ and $\|v_0^u\| \leq 10^{-2} Q(x)<Q(x).$ Since $v_0^u=(\sigma _x^s \circ \sigma _x^u)(v_0^u)=\sigma _x^s (v_0^s)$ and

$$ \begin{align*} \|v_0^s\|\leq\|\sigma_x^u(0)\|+\operatorname{Lip}(\sigma_x^u)\|v_0^u\| \leq10^{-3}Q(x)+\sqrt{\varepsilon}\cdot10^{-2}Q(x)\leq10^{-2}Q(x)<Q(x), \end{align*} $$

we have $P \in V_x^{s}$ . Moreover, we also see that $\|w\|\leq \|v_0^u\|+\|v_0^s\| \leq 50^{-1} Q(x)<d(x,\partial O)$ , and thus $P\in O$ .

To prove the uniqueness in the bigger ball $B_x^u(Q(x))$ , we note that $\sigma _x^s \circ \sigma _x^u$ maps $B_x^u(Q(x))$ into itself if $\varepsilon>0$ is small enough, and the same calculation as above shows that such a map has a unique fixed point even in $B_x^u(Q(x))$ .

(2) Now we verify that P is a Lipschitz function of $V_x^{u}, V_x^{s}$ . For every $x\in O$ , suppose $V_{i}^{t}\in \mathscr {V}_x^{t}$ are represented by $\sigma ^t_{i}$ , $i=1,2$ . Let $P_{i}=\exp _{x}(w_i)=\exp _{x}(v^u_{i}, v^s_{i})$ denote the intersection points of $V_{i}^{u} \cap V_{i}^{s}$ . We saw above that $v^s_{i}=\sigma ^u_{i}(v^u_{i})$ and that $v^u_{i}=\sigma ^s_{i}(v^s_{i})$ because $v^u_{i}$ is a fixed point of $\sigma ^s_{i}\circ \sigma ^u_{i}$ .

Since $\exp _x$ is 2-Lipschitz, this gives that $d(P_1,P_2)\leq 2\|w_1-w_2\|$ . We have

$$ \begin{align*} \|w_1-w_2\|&\leq\|v^u_1-v^u_2\|+\|v^s_1-v^s_2\|\notag\\ &=\|\sigma_1^s(v^s_1)-\sigma_2^s(v^s_2)\|+\|\sigma_1^u(v^u_1)-\sigma_2^u(v^u_2)\|\notag\\ &\leq\|\sigma_1^s(v^s_1)-\sigma_1^s(v^s_2)\|+\|\sigma_1^s(v^s_2)-\sigma_2^s(v^s_2)\|\\&\quad+\|\sigma_1^u(v^u_1)-\sigma_1^u(v^u_2)\|+\|\sigma_1^u(v^u_2)-\sigma_2^u(v^u_2)\|\notag\\ &\leq\sqrt{\varepsilon}(\|v^s_1-v^s_2\|+\|v^u_1-v^u_2\|)+\|\sigma_1^s-\sigma_2^s\|_{C^0}+\|\sigma_1^u-\sigma_2^u\|_{C^0}. \end{align*} $$

Therefore, we conclude that

$$ \begin{align*} \begin{aligned} d(P_1,P_2)&\leq2( \|v^u_1-v^u_2\|+\|v^s_1-v^s_2\|)\notag\\ &\leq\frac{2}{1-\sqrt{\varepsilon}}(d_{C^0}(V^u_1,V^u_2)+d_{C^0}(V^s_1,V^s_2)). \end{aligned}\\[-43pt] \end{align*} $$

Although the spaces $\mathscr {V}^{t}$ and the action of f or $f^{-1}$ are hard to work with due to the nonlinearity, from the definition of admissible manifold, through the inverse of the exponential map, the action of f or $f^{-1}$ on an admissible manifold can be locally lifted to the tangent space. For example, for the action of f, if $V_x^u$ is a u-admissible manifold at x, then $f(V_x^u)=\exp _{y}\{F_{x,y}(v_x^u,\sigma ^u_x(v_x^u)):\|v_x^u\|\leq Q(x)\}$ if $d(f(x),y)<\delta ^u(\varepsilon (x))$ , where $\delta ^u(\cdot )$ is given by Proposition 3.1. To prove that $f(V_x^u)$ contains a u-admissible manifold $V_y^u$ at y, we write $F_{x,y}|_{S_x}=D_0F_{x,y}+\phi _{x,y}$ in the form

(4.2) $$ \begin{align} F_{x,y}(v_x^u,\sigma^u_x(v_x^u))=(G_{x,y}^{\sigma^u_x}(v_x^u),L_{x,y}^{\sigma^u_x}(v_x^u)), \end{align} $$

where

(4.3) $$ \begin{align} G_{x,y}^{\sigma^u_x}(\cdot):&=D^{uu}_{x,y}(\cdot)+D^{us}_{x,y}\circ\sigma_x^u(\cdot)+\phi^u_{x,y}(\cdot,\sigma_x^u(\cdot)),\notag\\ L_{x,y}^{\sigma^u_x}(\cdot):&=D^{ss}_{x,y}\circ\sigma_x^u(\cdot)+D^{su}_{x,y}(\cdot)+\phi^s_{x,y}(\cdot,\sigma_x^u(\cdot)). \end{align} $$

If $B_y^u(Q(y))\subset G_{x,y}^{\sigma ^u_x}(B_x^u(Q(x)))$ and $G_{x,y}^{\sigma ^u_x}$ is injective, we can define $\sigma _y^u:=L_{x,y}^{\sigma _x^u}\circ (G_{x,y}^{\sigma _x^u})^{-1}$ , and we have

$$ \begin{align*} \begin{aligned} f(V_x^u)&=\exp_{y}\{(G_{x,y}^{\sigma_x^u}(v_x^u),\ L_{x,y}^{\sigma_x^u}\circ(G_{x,y}^{\sigma_x^u})^{-1}\circ G_{x,y}^{\sigma_x^u}(v_x^u)):\|v_x^u\|\leq Q(x)\}\notag\\ &\supset\exp_y\{(v_y^u,\sigma_y^u(v_y^u)):\|v_y^u\|\leq Q(y)\}, \end{aligned} \end{align*} $$

that is, $f(V_x^u)$ contains a u-admissible manifold $V_y^u=\exp _y\{(v_y^u,\sigma _y^u(v_y^u)):\|v_y^u\|\leq Q(y)\}$ when $\sigma _y^u$ satisfies properties (AM1)–(AM3). If $V_y^u$ obtained in this way is unique, then the graph transform $\mathscr {F}_{x,y}^{u}$ (see Definition 4.4 below) sends a u-admissible manifold at x with representing function $\sigma _x^u$ to a u-admissible manifold at y whose graph of the representing function $\sigma _y^u$ is contained in the action of $F_{x,y}$ on the graph of $\sigma _x^u$ .

Similarly, when $d(f^{-1}(y), x)<\delta ^s(\varepsilon (y))$ , the case of $f^{-1}(V_y^s)$ is symmetric and the corresponding graph transform $\mathscr {F}_{x,y}^{s}$ maps an s-admissible manifold at y to an s-admissible manifold at x.

We start with a definition and a basic lemma which will be used many times throughout the paper.

Definition 4.3. For $x,y\in O$ , the edge $x\rightarrow y$ means

$$ \begin{align*} d(f(x),y)<\delta^u(\varepsilon(x))Q(x)^2Q(f(x))\quad \text{and} \quad d(f^{-1}(y),x)<\delta^s(\varepsilon(y))Q(y)^2Q(f^{-1}(y)). \end{align*} $$

Lemma 4.1. Fix any positive constants $C_1, C_2, C_3, C_4$ , and suppose $x\rightarrow y$ . If $\varepsilon>0$ is small enough, we have:

  1. (1) $C_1Q(y)+d(f(x),y)\leq C_1Q(x)(m(Df|_{E^u(x)})^\kappa -C_2\varepsilon \varepsilon (x))$ ;

  2. (2) $C_3Q(y)-d(f(x),y)\geq C_3Q(x)(\|Df|_{E^s(x)}\|^\kappa +C_4\varepsilon \varepsilon (x))$ .

A similar statement holds for $f^{-1}$ .

Proof. We give the proof for part (1), the proof of part (2) follows in a similar manner and is left to the reader.

First, we fix

$$ \begin{align*} 0<\varepsilon\leq\min\bigg\{1,\frac{1}{\gamma-1},(2\gamma C_1)^{-({\alpha-\delta})/{2}}, \bigg(\frac{C_1}{2}\bigg)^{({\alpha-\delta})/{4}}, \frac{C-1}{1+C_2}\bigg\}. \end{align*} $$

Since $d(f(x),y)<\delta ^u(\varepsilon (x))Q(x)^2Q(f(x))$ , we have $({d(f(x),y)}/{d(f(x),\partial O)})<\delta ^u(\varepsilon (x))Q(x)^2<\varepsilon $ . By the fact that $(1+a)^\gamma \leq 1+2\gamma a$ if $0<a\leq ({1}/({\gamma -1}))$ , we obtain

$$ \begin{align*} \begin{aligned} Q(y)&\leq\varepsilon^{{2}/({\alpha-\delta})}\min\{r_0^\gamma,(d(f(x),\partial O)+d(y,f(x)))^\gamma\}\notag\\ &\leq\varepsilon^{{2}/({\alpha-\delta})}\min\bigg\{r_0^\gamma,d(f(x),\partial O)^\gamma\bigg(1+2\gamma\frac{d(y,f(x))}{d(f(x),\partial O)}\bigg)\bigg\}\notag\\ &\leq Q(f(x))+2\gamma\varepsilon^{{2}/({\alpha-\delta})}d(y,f(x))\notag\\ &\leq Q(f(x))+ \frac{d(y,f(x))}{C_1}. \end{aligned} \end{align*} $$

Recall that $0<\delta ^u(\varepsilon (x))<\varepsilon \varepsilon (x)$ in Proposition 3.1 and using Lemma 3.2, we have

$$ \begin{align*} \begin{aligned} &\frac{C_1Q(y)+d(f(x),y)+C_1C_2\varepsilon\varepsilon(x)Q(x)}{C_1Q(x)}\\ &\quad\leq\frac{Q(f(x))}{Q(x)}+\frac{2d(y,f(x))}{C_1Q(x)}+C_2\varepsilon\varepsilon(x)\notag\\ &\quad\leq\frac{Q(f(x))}{Q(x)}+\frac{2}{C_1}\varepsilon^{{4}/({\alpha-\delta})}\delta^u(\varepsilon(x))+C_2\varepsilon\varepsilon(x)\notag\\ &\quad\leq \frac{1}{C}(m(Df|_{E^u(x)})^\kappa-1)+1+(1+C_2)\varepsilon\varepsilon(x)\notag\\ &\quad\leq \frac{1}{C}(m(Df|_{E^u(x)})^\kappa-1)+1+\frac{C-1}{C}(m(Df|_{E^u(x)})^\kappa-1)\notag\\ &\quad=m(Df|_{E^u(x)})^\kappa, \end{aligned} \end{align*} $$

proving part (1).

Proposition 4.2. The following hold for all $\varepsilon>0$ small enough. Suppose $x\rightarrow y$ , then:

  1. (1) the map $G_{x,y}^{\sigma _x^u}:B_x^u(Q(x))\rightarrow E^u(y)$ defined by

    $$ \begin{align*}&G_{x,y}^{\sigma_x^u}(v^u_x)\\ &\quad=D_{x,y}^{uu}(v^u_x)+D_{x,y}^{us}\circ\sigma^u_x(v^u_x)+\phi_{x,y}^u(v^u_x,\sigma^u_x(v^u_x))\quad \text{for all } v^u_x\in B_x^u(Q(x)),\end{align*} $$

    is injective, and $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))\supset B_y^u(Q(y))$ ;

  2. (2) the map $\sigma _y^u:=L_{x,y}^{\sigma _x^u}\circ (G_{x,y}^{\sigma _x^u})^{-1}$ defined on $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ satisfies properties (AM1)–(AM3), where the map $L_{x,y}^{\sigma ^u_x}:B_x^u(Q(x))\rightarrow E^u(y)$ is defined by

    $$ \begin{align*}L_{x,y}^{\sigma^u_x}(v^u_x)&:=D^{ss}_{x,y}\circ\sigma_x^u(v^u_x)\\ &\quad+D^{su}_{x,y}(v^u_x)+\phi^s_{x,y}(v^u_x,\sigma_x^u(v^u_x))\quad \text{for all } v^u_x\in B_x^u(Q(x)).\end{align*} $$

    The symmetric statement holds for $F_{x,y}^{-1}$ .

Proof. The proof is a straightforward adaption of arguments in [Reference Sarig22, Proposition 4.12]. We give the proof in the case of $F_{x,y}$ . The case of $F_{x,y}^{-1}$ is symmetric.

(1) The well-defined nature of $(G_{x,y}^{\sigma _x^u})^{-1}$ is a consequence of the expansion property of $Df|_{E^u(x)}$ . For every $v_x^u\in B_x^u(Q(x))$ , by property (AM2), we know that $\|D_{v_x^u}{\sigma ^u_x}\|\leq 1$ if $0<\varepsilon \leq \min \{1,{C}/{4}\}$ . Therefore, from Proposition 3.1(2) and Lemma 3.1, we have

$$ \begin{align*} \begin{aligned} \|D_{v_x^u}G_{x,y}^{\sigma^u_x}\|&\geq m(D_{x,y}^{uu})-\|D_{x,y}^{us}\|\ \|D_{v_x^u}{\sigma^u_x}\|-\|D_{(v_x^u,\sigma^u_x(v_x^u))}\phi^u_{x,y}\|(1+\|D_{v_x^u}{\sigma^u_x}\|)\notag\\ &\geq m(Df|_{E^{u}(x)})-\varepsilon\varepsilon(x)-\varepsilon\varepsilon(x)-2\varepsilon\varepsilon(x)\notag\\ &\geq m(Df|_{E^{u}(x)})^\kappa-4\varepsilon\varepsilon(x)>1. \end{aligned} \end{align*} $$

It follows that $G_{x,y}^{\sigma ^u_x}$ is $[m(Df|_{E^{u}(x)})-4\varepsilon \varepsilon (x)]$ -expanding and hence one-to-one, and $(G_{x,y}^{\sigma _x^u})^{-1}$ is well defined on $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ .

By invariance of the domain, to prove $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))\supset B_y^u(Q(y))$ , the problem reduces to show that

$$ \begin{align*} \|G_{x,y}^{\sigma^u_x}(v_x^u)\|\geq Q(y) \end{align*} $$

for any $v_x^u\in \partial B_x^u(Q(x))$ .

According to

$$ \begin{align*} \begin{aligned} \|G_{x,y}^{\sigma^u_x}(0)\|&=\|D_{x,y}^{us}\circ\sigma^u_x(0)+\phi^u_{x,y}(0,\sigma^u_x(0))\|\notag\\ &\leq\|D_{x,y}^{us}\|\ \|\sigma^u_x(0)\|+\|\phi_{x,y}(0,0)\|+\operatorname{Lip}(\phi_{x,y})\|\sigma^u_x(0)\|,\\ \end{aligned} \end{align*} $$

by property (AM1) and Proposition 3.1(2), we have

(4.4) $$ \begin{align} \|G_{x,y}^{\sigma^u_x}(0)\|\leq2\varepsilon\varepsilon(x)\times 10^{-3}Q(x)+d(f(x),y). \end{align} $$

In particular, using Lemma 4.1 for $C_1=1, C_2=5$ , and the fact that $G_{x,y}^{\sigma ^u_x}$ is $[m(Df|_{E^{u}(x)})-4\varepsilon \varepsilon (x)]$ -expanding, we have that for any $v_x^u\in \partial B_x^u(Q(x))$ ,

$$ \begin{align*} \begin{aligned} \|G_{x,y}^{\sigma^u_x}(v_x^u)\|&\geq \|G_{x,y}^{\sigma^u_x}(v_x^u)-G_{x,y}^{\sigma^u_x}(0)\|-\|G_{x,y}^{\sigma^u_x}(0)\|\notag\\ &\geq (m(Df|_{E^{u}(x)})-4\varepsilon\varepsilon(x))Q(x)-2\varepsilon\varepsilon(x)\times 10^{-3}Q(x)-d(f(x),y)\notag\\ &\geq (m(Df|_{E^{u}(x)})^\kappa-5\varepsilon\varepsilon(x))Q(x)-d(f(x),y)\notag\\ &\geq Q(y). \end{aligned} \end{align*} $$

(2) We first prove $\sigma ^u_y$ satisfies property (AM1). Denote $v_{0x}^u:=(G_{x,y}^{\sigma ^u_x})^{-1}(0)$ , since $G_{x,y}^{\sigma ^u_x}$ is $[m(Df|_{E^{u}(x)})-4\varepsilon \varepsilon (x)]$ -expanding on $B_x^u(Q(x))$ , in particular,

$$ \begin{align*} \|D_{v_y^u}(G_{x,y}^{\sigma^u_x})^{-1})\|<1\quad \text{for all } v_y^u\in G_{x,y}^{\sigma_x^u}(B_x^u(Q(x))). \end{align*} $$

By equation (4.4), we have

$$ \begin{align*} \begin{aligned} \|v_{0x}^u\|&=\|(G_{x,y}^{\sigma^u_x})^{-1}(0)-(G_{x,y}^{\sigma^u_x})^{-1}\circ G_{x,y}^{\sigma^u_x}(0)\|\notag\\ &\leq\|D(G_{x,y}^{\sigma^u_x})^{-1})\|_{C^0}\|G_{x,y}^{\sigma^u_x}(0)\|\notag\\ &\leq2\varepsilon\varepsilon(x)\times 10^{-3}Q(x)+d(f(x),y)\notag\\ &\leq3\varepsilon\varepsilon(x)\times 10^{-3}Q(x). \end{aligned} \end{align*} $$

Note that from equation (3.6) of Lemma 3.2, it follows that $\|D_{x,y}^{ss}\|\leq \|Df|_{E^s(x)}\|^\kappa +\varepsilon \varepsilon (x)\leq 1$ if $0<\varepsilon \leq \min \{1,C\}$ . According to properties (AM1), (AM2), and Lemma 4.1 for $C_3=10^{-3}, C_4=13$ , we obtain

$$ \begin{align*} \begin{aligned} \|\sigma^u_y(0)\|&=\|L_{x,y}^{\sigma_x^u}(v_{0x}^u)\|\notag\\ &=\|D_{x,y}^{ss}\circ\sigma_x^u(v_{0x}^u)+D_{x,y}^{su}(v_{0x}^u)+ \phi_{x,y}^s(v_{0x}^u,\sigma_x^u(v_{0x}^u))\|\notag\\ &\leq\|D_{x,y}^{ss}\|(\|\sigma_x^u(0)\|+\operatorname{Lip}(\sigma_x^u)\|v_{0x}^u\|)+\|D_{x,y}^{su}\|\ \|v_{0x}^u\|+ \|\phi_{x,y}^s(0,0)\|\\&\quad+\operatorname{Lip}(\phi^s_{x,y})(1+\operatorname{Lip}(\sigma_x^u))\|v_{0x}^u\|\notag\\ &\leq(\|Df|_{E^s(x)}\|^\kappa+\varepsilon\varepsilon(x))10^{-3}Q(x)+12\varepsilon\varepsilon(x)\times 10^{-3}Q(x)+d(f(x),y)\notag\\ &\leq 10^{-3}Q(y), \end{aligned} \end{align*} $$

proving property (AM1).

Next we prove $\|D\sigma ^u_y\|_{C^0}\leq \sqrt {\varepsilon }$ , where the norm is taken in $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ .

For all $v_y^u\in G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ , $v_x^u=(G_{x,y}^{\sigma _x^u})^{-1}(v_y^u)\in B_x^u(Q(x))$ . Thanks to $\|D_{v_y^u} (G_{x,y}^{\sigma ^u_x})^{-1})\|<1$ , property (AM2) is easy to be verified from

$$ \begin{align*} \begin{aligned} \|D_{v_y^u}\sigma^u_y\|&=\|D_{x,y}^{ss}\cdot D_{v_{x}^u}\sigma_x^u\cdot D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}+D_{x,y}^{su}\cdot D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\\&\quad+ D_{v_{x}^u}\phi_{x,y}^s\cdot D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\|\notag\\ &\leq\|D_{x,y}^{ss}\|\ \|D\sigma_x^u\|_{C^0}+3\varepsilon\varepsilon(x)\notag\\ &\leq\|Df|_{E^s(x)}\|\sqrt{\varepsilon}+4\varepsilon\varepsilon(x)\notag\\ &\leq\sqrt{\varepsilon} \end{aligned} \end{align*} $$

if $0<\varepsilon \leq \min \{1,({C}/{4})^2\}$ .

Finally, we have to show that $\sigma ^u_y$ satisfies property (AM3) also. From

$$ \begin{align*} \sigma_y^u=L_{x,y}^{\sigma_x^u}\circ(G_{x,y}^{\sigma_x^u})^{-1} =[D^{ss}_{x,y}\circ\sigma_x^u(\cdot)+D^{su}_{x,y}(\cdot)+\phi^s_{x,y}(\cdot,\sigma_x^u(\cdot))]\circ(G_{x,y}^{\sigma_x^u})^{-1}, \end{align*} $$

we have

$$ \begin{align*} \begin{aligned} \|D\sigma_y^u\|_{C^{\delta/2}}&=\|(D^{ss}_{x,y}\cdot D\sigma_x^u+D^{su}_{x,y} +D\phi^s_{x,y})\cdot D(G_{x,y}^{\sigma_x^u})^{-1}\|_{C^{\delta/2}}\notag\\ &\leq(\|D^{ss}_{x,y}\|\cdot \|D\sigma_x^u\|_{C^{\delta/2}}+\|D^{su}_{x,y}\|+2\|D\phi_{x,y}\|_{C^{\delta/2}(S_x)}) \|D(G_{x,y}^{\sigma_x^u})^{-1}\|_{C^{\delta/2}}.\notag\\ \end{aligned} \end{align*} $$

Claim. If $\varepsilon>0$ is small enough, $\|D(G^{\sigma _x^u}_{x,y})^{-1}\|_{C^{\delta /2}}<1$ .

Proof of Claim

For $v_y^u,w_y^u\in G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ , notice that $D_{v_y^u}(G_{x,y}^{\sigma _x^u})^{-1}\cdot D_{v_x^u}G_{x,y}^{\sigma _x^u}$ and $D_{w_x^u}G_{x,y}^{\sigma _x^u}\cdot D_{w_y^u}(G_{x,y}^{\sigma _x^u})^{-1}$ are identity maps, where $v_y^u=G_{x,y}^{\sigma _x^u}(v_x^u)$ , $w_x^u=(G_{x,y}^{\sigma _x^u})^{-1}(w_y^u)$ . Thus, we have

$$ \begin{align*} \begin{aligned} &\|D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}-D_{w_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\|\notag\\ &\quad=\|D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\cdot(D_{w_x^u}G_{x,y}^{\sigma_x^u}-D_{v_x^u}G_{x,y}^{\sigma_x^u})\cdot D_{w_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\|\notag\\ &\quad=\|D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\cdot(D_{x,y}^{us}D_{w_x^u}\sigma_x^u+D_{w_x^u}\phi_{x,y}^u\\&\qquad-D_{x,y}^{us}D_{v_x^u}\sigma_x^u-D_{v_x^u}\phi_{x,y}^u)\cdot D_{w_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\|. \end{aligned} \end{align*} $$

First, to estimate $\|D_{w_x^u}\phi _{x,y}^u-D_{v_x^u}\phi _{x,y}^u\|$ in parentheses, a little manipulation is needed. If $0<\varepsilon \leq 1$ , by property (AM3) and Proposition 3.1(3), we can get

$$ \begin{align*} \begin{aligned} &\|D_{w_x^u}\phi^u_{x,y}(\cdot,\sigma_x^u(\cdot))-D_{v_x^u}\phi^u_{x,y}(\cdot,\sigma_x^u(\cdot))\|\notag\\ &\quad=\left\|D_{(w_x^u,\sigma_x^u(w_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{w_x^u}\sigma_x^u \end{array}\right]-D_{(v_x^u,\sigma_x^u(v_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_x^u}\sigma_x^u \end{array}\right]\right\|\notag\\ &\quad\leq\left\|D_{(w_x^u,\sigma_x^u(w_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{w_x^u}\sigma_x^u \end{array}\right]-D_{(w_x^u,\sigma_x^u(w_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_x^u}\sigma_x^u \end{array}\right]\right\|\notag\\ &\qquad+\left\|D_{(w_x^u,\sigma_x^u(w_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_x^u}\sigma_x^u \end{array}\right]-D_{(v_x^u,\sigma_x^u(v_x^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_x^u}\sigma_x^u \end{array}\right]\right\|\notag\\ &\quad\leq\frac{\varepsilon\varepsilon(x)}{2}\|w_x^u-v_x^u\|^{\delta/2}+4\varepsilon\varepsilon(x)\|w_x^u-v_x^u\|^{\delta/2}\notag\\ &\quad=\frac{9\varepsilon\varepsilon(x)}{2}\|w_x^u-v_x^u\|^{\delta/2}. \end{aligned} \end{align*} $$

For the rest in the parentheses, from property (AM3), we find

$$ \begin{align*} \|D_{x,y}^{us}D_{w_x^u}\sigma_x^u-D_{x,y}^{us}D_{v_x^u}\sigma_x^u\|\leq\tfrac{1}{2}\varepsilon\varepsilon(x)\|w_x^u-v_x^u\|^{\delta/2}; \end{align*} $$

therefore, we obtain that

$$ \begin{align*} \begin{aligned} &\|D_{v_y^u}(G_{x,y}^{\sigma_x^u})^{-1}-D_{w_y^u}(G_{x,y}^{\sigma_x^u})^{-1}\|\notag\\ &\quad\leq \|D(G_{x,y}^{\sigma_x^u})^{-1}\|^2_{C^0}\ 5\varepsilon\varepsilon(x)\|w_x^u-v_x^u\|^{\delta/2}\notag\\ &\quad\leq 5\varepsilon\varepsilon(x)\|D(G_{x,y}^{\sigma_x^u})^{-1}\|^{2+{\delta}/{2}}_{C^0}\|w_y^u-v_y^u\|^{\delta/2} \end{aligned} \end{align*} $$

or

$$ \begin{align*} \operatorname{Hol}_{\delta/2}(D(G^{\sigma_x^u}_{x,y})^{-1})\leq5\varepsilon\varepsilon(x)\|D(G_{x,y}^{\sigma_x^u})^{-1}\|^{2+{\delta}/{2}}_{C^0}\leq5\varepsilon\varepsilon(x). \end{align*} $$

Using $G_{x,y}^{\sigma ^u_x}$ is $[m(Df|_{E^{u}(x)})-4\varepsilon \varepsilon (x)]$ -expanding again, that is,

$$ \begin{align*} \|D(G_{x,y}^{\sigma^u_x})^{-1}\|_{C^0}\leq\frac{1}{m(Df|_{E^{u}(x)})-4\varepsilon\varepsilon(x)}, \end{align*} $$

we get finally

$$ \begin{align*} \begin{aligned} \|D(G^{\sigma_x^u}_{x,y})^{-1}\|_{C^{\delta/2}}&=\|D(G^{\sigma_x^u}_{x,y})^{-1}\|_{C^0}+ \operatorname{Hol}_{\delta/2}(D(G^{\sigma_x^u}_{x,y})^{-1})\notag\\ &\leq\frac{1}{m(Df|_{E^{u}(x)})-4\varepsilon\varepsilon(x)}+5\varepsilon\varepsilon(x)\notag\\ &<1 \end{aligned} \end{align*} $$

if $0<\varepsilon <\min \{1,{C}/{5(C^f+4)}\}$ . This completes the proof of the claim.

We are now turning to the proof of $\|D\sigma _y^u\|_{C^{\delta /2}}\leq \tfrac 12$ . From Proposition 3.1(2) and (3), we have $\|D\phi _{x,y}\|_{C^{\delta /2}(S_x)}\leq 2\varepsilon \varepsilon (x)$ . By using equation (3.6) of Lemma 3.2 and combining with the claim above, we obtain that

$$ \begin{align*} \begin{aligned} \|D\sigma_y^u\|_{C^{\delta/2}}&\leq(\|D^{ss}_{x,y}\|\cdot \|D\sigma_x^u\|_{C^{\delta/2}}+\|D^{su}_{x,y}\|+2\|D\phi_{x,y}\|_{C^{\delta/2}(S_x)}) \|D(G_{x,y}^{\sigma_x^u})^{-1}\|_{C^{\delta/2}}\notag\\ &\leq\|D^{ss}_{x,y}\|\cdot \|D\sigma_x^u\|_{C^{\delta/2}}+\|D^{su}_{x,y}\|+2\|D\phi_{x,y}\|_{C^{\delta/2}(S_x)}\notag\\ &\leq\tfrac{1}{2}(\|Df|_{E^s(x)}\|+\varepsilon\varepsilon(x))+5\varepsilon\varepsilon(x)\notag\\ &\leq \tfrac{1}{2} \end{aligned} \end{align*} $$

when $0<\varepsilon \leq \min \{1, {C}/{11}\}$ , and the proof of this proposition is completed.

As has been said, since

$$ \begin{align*} f(V_x^u)=\exp_{y}\{(G_{x,y}^{\sigma_x^u}(v_x^u),\ \sigma_y^u\circ G_{x,y}^{\sigma_x^u}(v_x^u)):\|v_x^u\|\leq Q(x)\} \end{align*} $$

and $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))\supset B_y^u(Q(y))$ , Proposition 4.2 above shows that $f(V_x^u)$ restricts to a unique u-admissible manifold $\widehat {V}_y^u$ at y, where

$$ \begin{align*} \widehat{V}_y^u=\exp_{y}\{(v_y^u,\sigma_y^u(v_y^u)):\|v_y^u\|\leq Q(y)\}. \end{align*} $$

Thus, we can summarize what we have proved as the following definition which is well defined for $\varepsilon>0$ small enough.

Definition 4.4. Suppose $x\rightarrow y$ .

  1. (1) The unstable graph transform $\mathscr {F}_{x,y}^{u}: \mathscr {V}_x^{u} \rightarrow \mathscr {V}_y^{u} $ is the map that sends $V_x^{u} \in \mathscr {V}_x^{u}$ to the unique $\mathscr {F}_{x,y}^{u}[V_x^{u}] \in \mathscr {V}_y^{u}$ with representing function $\sigma _y^u$ such that $\mathscr {F}_{x,y}^{u}[V_x^{u}]=\exp _{y}\{(v^u, \sigma _y^u(v^u)):\|v^u\| \leq Q(y)\}\subset f(V_x^{u})$ .

  2. (2) The stable graph transform $\mathscr {F}_{x,y}^{s}: \mathscr {V}_y^{s} \rightarrow \mathscr {V}_x^{s} $ is the map that sends $V_y^{s} \in \mathscr {V}_x^{s}$ to the unique $\mathscr {F}_{x,y}^{s}[V_y^{s}] \in \mathscr {V}_x^{s}$ with representing function $\sigma _x^s$ such that $\mathscr {F}_{x,y}^{s}[V_{y}^{s}]=\exp _{x}\{(\sigma _x^s(v^s), v^s):\|v^s\| \leq Q(x)\}\subset f^{-1}(V_y^{s})$ .

Corollary 4.1. The following holds for $\varepsilon>0$ small enough. Suppose $x\rightarrow y$ and $V_x^u\in \mathscr {V}_{x}^u$ . Then:

  1. (1) if $V_x^u$ is represented by the function $\sigma ^u_x$ and $p:=\exp _x(0,\sigma ^u_x(0))$ , then $f(p)\in \mathscr {F}_{x,y}^{u}[V_x^u]$ ;

  2. (2) $f(V_x^u)$ intersects any $V_y^s\in \mathscr {V}_{y}^s$ at a unique point.

Similar statements hold for the $f^{-1}$ -image of an s-admissible manifold at y.

Proof.

  1. (1) Since $\mathscr {F}_{x,y}^{u}[V_x^u]=\exp _{y}\{(v_y^u,\sigma _y^u(v_y^u)):\|v_y^u\|\leq Q(y)\}$ , it suffices to check that

    $$ \begin{align*} F_{x,y}(0,\sigma^u_x(0))=(G_{x,y}^{\sigma_x^u}(0),L_{x,y}^{\sigma_x^u}(0))\in\{(v_y^u,\sigma_y^u(v_y^u)):\|v_y^u\|\leq Q(y)\}, \end{align*} $$
    or check $\|G_{x,y}^{\sigma _x^u}(0)\|\leq Q(y)$ , which is straightforward.
  2. (2) For any $V_y^s\in \mathscr {V}_{y}^s$ with the representing function $\sigma _y^s$ , by Proposition 4.1(1), $\mathscr {F}_{x,y}^{u}[V_x^u]$ and $V_y^s$ intersect at a single point. According to Definition 4.4, $f(V_x^u)$ contains a u-manifold $\mathscr {F}_{x,y}^{u}[V_x^u]\in \mathscr {V}_{y}^u$ ; therefore, $f(V_x^u)$ and $V_y^s$ intersect at least at one point.

Since

$$ \begin{align*} f(V_x^u)=\exp_{y}\{(v_y^u,\sigma_y^u(v_y^u)):v_y^u\in G_{x,y}^{\sigma_x^u}(B_x^u(Q(x)))\} \end{align*} $$

with $\operatorname {Lip}(\sigma _y^u)\leq \sqrt {\varepsilon }$ , by the Kirszbraun theorem, we can extend $\sigma _y^s$ to a Lipschitz function $\tilde {\sigma }_y^s$ on $G_{x,y}^{\sigma _x^u}(B_x^u(Q(x)))$ with $\operatorname {Lip}(\tilde {\sigma }_y^s)=\operatorname {Lip}(\sigma _y^s)\leq \sqrt {\varepsilon }$ . The extension represents a Lipschitz manifold $\tilde {V}_y^s\supset V_y^s$ . Hence, the proof is quite similar to that given earlier in Proposition 4.1(1) to conclude that $f(V_x^u)\cap \tilde {V}_y^s$ consists of a single point and so is omitted.

Proposition 4.3. If $\varepsilon>0$ is small enough, then the following hold. Suppose $x\rightarrow y$ , if $V^u_{1}, V^u_{2} \in \mathscr {V}_x^u$ , we have:

  1. (1) $d_{C^{0}}(\mathscr {F}^u_{x,y}(V^u_{1}), \mathscr {F}^u_{x,y}(V^u_{2})) \leq \|Df|_{E^s(x)}\|^{1/2} d_{C^{0}}(V^u_{1}, V^u_{2})$ ;

  2. (2) $d_{C^{1}}(\mathscr {F}^u_{x,y}(V^u_{1}), \mathscr {F}^u_{x,y}(V^u_{2})) \leq \|Df|_{E^s(x)}\|^{1/2} (d_{C^{1}}(V^u_{1}, V^u_{2})+d_{C^{0}}(V^u_{1}, V^u_{2})^{\delta /2})$ .

Similar statements hold for $\mathscr {F}^s_{x,y}$ .

Proof. The proof is similar to the proof of [Reference Sarig22, Proposition 4.14]. We prove the proposition for $\mathscr {F}^u_{x,y}$ and leave the case of $\mathscr {F}^s_{x,y}$ to the reader.

Let $V_{1}, V_{2}$ with representing functions $\sigma _{1}, \sigma _{2}$ , and let $\tilde {\sigma }_{1}, \tilde {\sigma }_{2}$ be the representing functions of $\mathscr {F}^u_{x,y}(V_{1}), \mathscr {F}^u_{x,y}(V_{2}),$ that is, $\tilde {\sigma }_{i}=L^{\sigma _i}_{x,y}\circ (G^{\sigma _i}_{x,y})^{-1}|_{B_y^u(Q(y))}$ , $i=1,2$ .

(1) For any $v_y^u\in B_y^u(Q(y))$ , denote $v_{1x}^u=(G^{\sigma _1}_{x,y})^{-1}(v_y^u)$ , $v_{2x}^u=(G^{\sigma _2}_{x,y})^{-1}(v_y^u)$ . Some tedious manipulation yields

$$ \begin{align*} \begin{aligned} &\|\tilde{\sigma}_{1}(v_y^u)-\tilde{\sigma}_{2}(v_y^u)\|=\|\tilde{\sigma}_{1}\circ G^{\sigma_1}_{x,y}(v_{1x}^u)-\tilde{\sigma}_{2}\circ G^{\sigma_1}_{x,y}(v_{1x}^u)\|\notag\\ &\quad\leq\|\tilde{\sigma}_{1}\circ G^{\sigma_1}_{x,y}(v_{1x}^u)-\tilde{\sigma}_{2}\circ G^{\sigma_2}_{x,y}(v_{1x}^u)\|+\|\tilde{\sigma}_{2}\circ G^{\sigma_2}_{x,y}(v_{1x}^u)-\tilde{\sigma}_{2}\circ G^{\sigma_1}_{x,y}(v_{1x}^u)\|\notag\\ &\quad\leq\|D_{x,y}^{ss}(\sigma_1(v_{1x}^u)-\sigma_2(v_{1x}^u))\|+\|\phi_{x,y}^s(v_{1x}^u,\sigma_1(v_{1x}^u))-\phi_{x,y}^s(v_{1x}^u,\sigma_2(v_{1x}^u))\|\\&\qquad+\operatorname{Lip}(\tilde{\sigma}_{2}) \|G^{\sigma_2}_{x,y}(v_{1x}^u)-G^{\sigma_1}_{x,y}(v_{1x}^u)\|\notag \end{aligned} \end{align*} $$
$$ \begin{align*} \begin{aligned} &\qquad+\operatorname{Lip}(\phi_{x,y})) \|\sigma_2(v_{1x}^u)-\sigma_1(v_{1x}^u)\|\notag\\ &\quad\leq(\|D_{x,y}^{ss}\|+\|D_{x,y}^{us}\|+ 2\operatorname{Lip}(\phi_{x,y}))\|\sigma_2(v_{1x}^u)-\sigma_1(v_{1x}^u)\|\notag\\ &\quad\leq(\|Df|_{E^s(x)}\|+6\varepsilon\varepsilon(x))\|\sigma_2(v_{1x}^u)-\sigma_1(v_{1x}^u)\|. \end{aligned} \end{align*} $$

We remind the reader that $C\varepsilon (x)\leq 1-\|Df|_{E^s(x)}\|^\kappa \leq 1-\|Df|_{E^s(x)}\|$ and introduce a new constant

(4.5) $$ \begin{align} a:=\inf_{x\in O}\frac{\|Df|_{E^s(x)}\|^{1/2}-\|Df|_{E^s(x)}\|}{1-\|Df|_{E^s(x)}\|}>0, \end{align} $$

then if $0<\varepsilon \leq ({aC}/{6})$ , we get finally

$$ \begin{align*} \begin{aligned} \|\tilde{\sigma}_{1}-\tilde{\sigma}_{2}\|_{C^0}&\leq(\|Df|_{E^s(x)}\|+aC\varepsilon(x))\|\sigma_{1}-\sigma_{2}\|_{C^0}\notag\\ &\leq\|Df|_{E^s(x)}\|^{1/2}\|\sigma_{1}-\sigma_{2}\|_{C^0}. \end{aligned} \end{align*} $$

(2) In view of part (1), our task now is to estimate $\|D\tilde {\sigma }_{1}- D\tilde {\sigma }_{2}\|_{C^{0}}$ in terms of $\|D\sigma _{1}-D\sigma _{2}\|_{C^{0}}$ and $\|\sigma _{1}-\sigma _{2}\|_{C^{0}}^{\delta /2}$ . We will show that

$$ \begin{align*} \begin{aligned} &\|D\tilde{\sigma}_{1}-D\tilde{\sigma}_{2}\|_{C^0}\notag\\ &\quad\leq(\|Df|_{E^s(x)}\|+3\varepsilon\varepsilon(x))\|D\sigma_1-D\sigma_2\|_{C^0} +\tfrac{1}{2}(\|Df|_{E^s(x)}\|+25\varepsilon\varepsilon(x))\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}. \end{aligned} \end{align*} $$

For any $v_y^u\in B_y^u(Q(y))$ , let $v_{ix}^u=(G^{\sigma _i}_{x,y})^{-1}(v_y^u)$ as part (1), where $i=1,2$ . We have

$$ \begin{align*} \begin{aligned} &\|D_{v_y^u}\tilde{\sigma}_{1}-D_{v_y^u}\tilde{\sigma}_{2}\|\notag\\ &\quad=\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_2}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1} -D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\\ &\qquad+\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\qquad+\|D_{v_{2x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_2}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|, \end{aligned} \end{align*} $$

so we need to estimate each term above. We divide our proof of part (2) into four steps.

First, note that the last term is easy to estimate because $\|D(G_{x,y}^{\sigma _2})^{-1}\|<1$ and $L_{x,y}^{\sigma _1}(\cdot )=D^{ss}_{x,y}\circ \sigma _1(\cdot )+D^{su}_{x,y}(\cdot )+\phi ^s_{x,y}(\cdot ,\sigma _1(\cdot ))$ ,

$$ \begin{align*} \begin{aligned} &\|D_{v_{2x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_2}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq \|D_{v_{2x}^u}L^{\sigma_1}_{x,y} -D_{v_{2x}^u}L^{\sigma_2}_{x,y}\|\notag\\ &\quad\leq\|D^{ss}_{x,y}\|\cdot\|D_{v_{2x}^u}\sigma_1-D_{v_{2x}^u}\sigma_2\| +\|D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))-D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_2(\cdot))\|. \end{aligned} \end{align*} $$

However, if $0<\varepsilon \leq 1$ , using Proposition 3.1(2), (3), and property (AM3), we get

$$ \begin{align*} \begin{aligned} &\|D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))-D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_2(\cdot))\|\notag\\ &\quad=\left\|D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]-D_{(v_{2x}^u,\sigma_2(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_2 \end{array}\right]\right\|\notag \end{aligned} \end{align*} $$
$$ \begin{align*} \begin{aligned} &\quad\leq\left\|D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]-D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_2 \end{array}\right]\right\|\notag\\ &\qquad+\left\|D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_2 \end{array}\right]-D_{(v_{2x}^u,\sigma_2(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_2 \end{array}\right]\right\|\notag\\ &\quad\leq\varepsilon\varepsilon(x)\|D\sigma_1-D\sigma_2\|_{C^0}+4\varepsilon\varepsilon(x)\|\sigma_1-\sigma_2\|^{\delta/2}_{C^0}. \end{aligned} \end{align*} $$

Consequently, we infer that the last term satisfies

(4.6) $$ \begin{align} &\|D_{v_{2x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_2}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq(\|Df|_{E^s(x)}\|+2\varepsilon\varepsilon(x))\|D\sigma_1-D\sigma_2\|_{C^0}+4\varepsilon\varepsilon(x)\|\sigma_1-\sigma_2\|^{\delta/2}_{C^0}. \end{align} $$

The next thing to do is to estimate the second term:

$$ \begin{align*} \begin{aligned} &\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}-D_{v_{2x}^u}L^{\sigma_1}_{x,y}\|\notag\\ &\quad\leq\|D^{ss}_{x,y}\|\cdot\|D_{v_{1x}^u}\sigma_1-D_{v_{2x}^u}\sigma_1\| +\|D_{v_{1x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))-D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))\|. \end{aligned} \end{align*} $$

Similarly, if $0<\varepsilon \leq 1$ , using Proposition 3.1(2), (3), and property (AM3), we have

$$ \begin{align*} \begin{aligned} &\|D_{v_{1x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))-D_{v_{2x}^u}\phi^s_{x,y}(\cdot,\sigma_1(\cdot))\|\notag\\ &\quad=\left\|D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]-D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\quad\leq\left\|D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]-D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\qquad+\left\|D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]-D_{(v_{2x}^u,\sigma_1(v_{2x}^u))}\phi^s_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{2x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\quad\leq\frac{\varepsilon\varepsilon(x)}{2}\|v_{1x}^u-v_{2x}^u\|^{\delta/2}+2\varepsilon\varepsilon(x)\|v_{1x}^u-v_{2x}^u\|^{\delta/2}\notag\\ &\quad=\frac{5\varepsilon\varepsilon(x)}{2}\|v_{1x}^u-v_{2x}^u\|^{\delta/2}. \end{aligned} \end{align*} $$

Due to $G_{x,y}^{\sigma _i}(\cdot )=D_{x,y}^{uu}(\cdot )+D_{x,y}^{us}\sigma _i(\cdot )+\phi _{x,y}^u(\cdot ,\sigma _i(\cdot ))$ , we obtain

(4.7) $$ \begin{align} \|v_{1x}^u-v_{2x}^u\|&=\|(G^{\sigma_1}_{x,y})^{-1}(v_y^u)-(G^{\sigma_2}_{x,y})^{-1}(v_y^u)\|\notag\\ &=\|(G^{\sigma_1}_{x,y})^{-1}\circ (G^{\sigma_2}_{x,y}\circ(G^{\sigma_2}_{x,y})^{-1}(v_y^u))-(G^{\sigma_1}_{x,y})^{-1}\circ(G^{\sigma_1}_{x,y}\circ(G^{\sigma_2}_{x,y})^{-1}(v_y^u))\|\notag\\ &\leq\|D(G^{\sigma_1}_{x,y})^{-1}\|_{C^0}\|G^{\sigma_2}_{x,y}(v_{2x}^u)-G^{\sigma_1}_{x,y}(v_{2x}^u)\|\notag\\ &\leq\|D_{x,y}^{us}\|\ \|\sigma_2(v_{2x}^u)-\sigma_1(v_{2x}^u)\|+\operatorname{Lip}(\phi_{x,y})\|\sigma_2(v_{2x}^u)-\sigma_1(v_{2x}^u)\|\notag\\ &\leq2\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}\notag\\ &\leq\|\sigma_2-\sigma_1\|_{C^0}.\end{align} $$

Hence, the second term is estimated as

(4.8) $$ \begin{align} &\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\circ D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1} -D_{v_{2x}^u}L^{\sigma_1}_{x,y}\circ D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D^{ss}_{x,y}\|\cdot\frac{1}{2}\|v_{1x}^u-v_{2x}^u\|^{\delta/2}+\frac{5\varepsilon\varepsilon(x)}{2}\|v_{1x}^u-v_{2x}^u\|^{\delta/2}\notag\\ &\quad\leq(\tfrac{1}{2}\|Df|_{E^s(x)}\|+3\varepsilon\varepsilon(x))\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}. \end{align} $$

Another step in the proof of part (2) is to establish an estimate of the first term. Since $\|D_{v_{1x}^u}L^{\sigma _1}_{x,y}\|<1$ and $\|D_{v_y^u}(G^{\sigma _i}_{x,y})^{-1}\|<1$ , $i=1,2$ , we have

$$ \begin{align*} \begin{aligned} &\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1} -D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1}-D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad=\|D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1}(D_{v_{2x}^u}G^{\sigma_2}_{x,y}-D_{v_{1x}^u}G^{\sigma_1}_{x,y})D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D_{v_{2x}^u}G^{\sigma_2}_{x,y}-D_{v_{1x}^u}G^{\sigma_2}_{x,y}\|+\|D_{v_{1x}^u}G^{\sigma_2}_{x,y}-D_{v_{1x}^u}G^{\sigma_1}_{x,y}\|. \end{aligned} \end{align*} $$

From the proof in property (AM3) of Proposition 4.2 and equation (4.7) above, we obtain that

$$ \begin{align*} \|D_{v_{2x}^u}G^{\sigma_2}_{x,y}-D_{v_{1x}^u}G^{\sigma_2}_{x,y}\|\leq5\varepsilon\varepsilon(x)\|v_{2x}^u-v_{1x}^u\|^{\delta/2}\leq5\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}. \end{align*} $$

At the same time, if $0<\varepsilon \leq 1$ , using Proposition 3.1(2), (3), and property (AM3), we get

$$ \begin{align*} \begin{aligned} &\|D_{v_{1x}^u}\phi^u_{x,y}(\cdot,\sigma_2(\cdot))-D_{v_{1x}^u}\phi^u_{x,y}(\cdot,\sigma_1(\cdot))\|\notag\\ &\quad=\left\|D_{(v_{1x}^u,\sigma_2(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_2 \end{array}\right]-D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\quad\leq\left\|D_{(v_{1x}^u,\sigma_2(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_2 \end{array}\right]-D_{(v_{1x}^u,\sigma_2(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\qquad+\left\|D_{(v_{1x}^u,\sigma_2(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]-D_{(v_{1x}^u,\sigma_1(v_{1x}^u))}\phi^u_{x,y}\left[\begin{array}{@{}c@{}} I \\ D_{v_{1x}^u}\sigma_1 \end{array}\right]\right\|\notag\\ &\quad\leq\varepsilon\varepsilon(x)\|D\sigma_2-D\sigma_1\|_{C^0}+2\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}. \end{aligned} \end{align*} $$

Hence, by using property (AM3) and equation (4.7) again, we get for this term that

(4.9) $$ \begin{align} &\|D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_1}_{x,y})^{-1} -D_{v_{1x}^u}L^{\sigma_1}_{x,y}\cdot D_{v_y^u}(G^{\sigma_2}_{x,y})^{-1}\|\notag\\ &\quad\leq\|D_{v_{2x}^u}G^{\sigma_2}_{x,y}-D_{v_{1x}^u}G^{\sigma_2}_{x,y}\|+\|D_{x,y}^{us}D_{v_{1x}^u}\sigma_2-D_{x,y}^{us}D_{v_{1x}^u}\sigma_2\|\notag\\ &\qquad+\|D_{v_{1x}^u}\phi^u_{x,y}(\cdot,\sigma_2(\cdot))-D_{v_{1x}^u}\phi^u_{x,y}(\cdot,\sigma_1(\cdot))\|\notag\\ &\quad\leq5\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|^{\delta/2}+\tfrac{1}{2}\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}\notag\\ &\qquad+\varepsilon\varepsilon(x)\|D\sigma_2-D\sigma_1\|_{C^0}+2\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}\notag\\ &\quad=\varepsilon\varepsilon(x)\|D\sigma_2-D\sigma_1\|_{C^0}+\frac{15}{2}\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}. \end{align} $$

Finally, plugging all estimates in equations (4.6), (4.8), and (4.9) together, it holds that

$$ \begin{align*} \begin{aligned} &\|D\tilde{\sigma}_{1}-D\tilde{\sigma}_{2}\|_{C^0}\notag\\ &\quad\leq\varepsilon\varepsilon(x)\|D\sigma_2-D\sigma_1\|_{C^0}+\frac{15}{2}\varepsilon\varepsilon(x)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}\notag\\ &\qquad+\big(\tfrac{1}{2}\|Df|_{E^s(x)}\|+3\varepsilon\varepsilon(x)\big)\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}\notag\\ &\qquad+(\|Df|_{E^s(x)}\|+2\varepsilon\varepsilon(x))\|D\sigma_1-D\sigma_2\|_{C^0}+4\varepsilon\varepsilon(x)\|\sigma_1-\sigma_2\|^{\delta/2}_{C^0}\notag\\ &\quad\leq(\|Df|_{E^s(x)}\|+3\varepsilon\varepsilon(x))\|D\sigma_1-D\sigma_2\|_{C^0} +\frac{1}{2}(\|Df|_{E^s(x)}\|+29\varepsilon\varepsilon(x))\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}\notag\\ &\quad\leq\|Df|_{E^s(x)}\|^{1/2}(\|D\sigma_1-D\sigma_2\|_{C^0}+\|\sigma_2-\sigma_1\|_{C^0}^{\delta/2}) \end{aligned} \end{align*} $$

if $0<\varepsilon \leq \min \{1,{aC}/{29}\}$ , where a is defined in equation (4.5). With the estimates of part (1), we conclude finally that

$$ \begin{align*} \|\tilde{\sigma}_{1}-\tilde{\sigma}_{2}\|_{C^1}\leq\|Df|_{E^s(x)}\|^{1/2}(\|\sigma_{1}-\sigma_{2}\|_{C^{1}} +\|\sigma_{1}-\sigma_{2}\|_{C^{0}}^{\delta/2}), \end{align*} $$

proving part (2).

5. Shadowing lemma and an infinite-to-one coding for f

Since O is second countable, we would like to replace O by a countable subset $\mathscr {A}$ which will be used to construct the set of vertices of a directed graph related to the dynamics of f.

Proposition 5.1. For all $\varepsilon>0$ sufficiently small, there exists a countable subset $\mathscr {A}\subset O$ with the following properties.

  1. (1) Discreteness: for all $r>0$ , the set $\{x \in \mathscr {A}: d(x,\partial O)\geq r\}$ is finite.

  2. (2) Sufficiency: for every $x \in O$ , there is a sequence $\{x_n\}_{n\in \mathbb {Z}}$ in $\mathscr {A}$ such that for every $n\in \mathbb {Z}$ :

    1. (a) $e^{-\beta \varepsilon }\leq ({\varepsilon (f^n(x))}/{\varepsilon (x_n)})\leq e^{\beta \varepsilon }$ and $e^{-\gamma \varepsilon }\leq ({Q(f^n(x))}/{Q(x_n)})\leq e^{\gamma \varepsilon }$ ;

    2. (b) $x_n\rightarrow x_{n+1}$ .

Proof. Fix a countable subset $\mathscr {A}$ of O such that

$$ \begin{align*} O=\bigcup_{z\in\mathscr{A}}B(z,r(z)), \end{align*} $$

where $r(z)=\varepsilon \min \{\delta ^u(\varepsilon \cdot \varepsilon (z)),\delta ^s(\varepsilon \cdot \varepsilon (z))\}\cdot Q(z)^2\cdot \min \{Q(f(z)),Q(f^{-1}(z))\}$ .

(1) For all $r>0$ , since $O(r)=\{x\in O: d(x,\partial O)\geq r\}$ is compact, if necessary, we can remove some elements of $\mathscr {A}$ in $O(r)$ to make the set $\{x \in \mathscr {A}: d(x,\partial O)\geq r\}$ finite and maintain the above denseness assumption.

(2) As mentioned above, we can fix a countable subset $\mathscr {A}$ of O such that $O=\bigcup _{z\in \mathscr {A}}B(z,r(z))$ and satisfying discreteness. For every $x\in O$ and any $n\in \mathbb {Z}$ , since $f^n(x)\in O$ , there exist $\{x_n\}_{n\in \mathbb {Z}}\in \mathscr {A}^{\mathbb {Z}}$ such that $d(f^n(x),x_{n})\leq r(x_n)$ for all $n\in \mathbb {Z}$ . For $\varepsilon>0$ sufficiently small, since $r(x_n)\leq ({\varepsilon }/{2}) Q(x_n)\leq ({\varepsilon }/{2}) d(x_n,\partial O)$ , it follows that

$$ \begin{align*} \begin{aligned} d(f^n(x),\partial O)&\leq d(f^n(x),x_n)+d(x_n,\partial O) \notag\\ &\leq e^\varepsilon d(x_n,\partial O), \end{aligned} \end{align*} $$

and hence

$$ \begin{align*} \varepsilon(f^n(x))\leq e^{\beta\varepsilon}\varepsilon(x_n)\quad\text{and}\quad Q(f^n(x))\leq e^{\gamma\varepsilon}Q(x_n). \end{align*} $$

Analogously, from $d(f^n(x),\partial O)\geq d(x_n,\partial O)-d(f^n(x),x_n)\geq e^{-\varepsilon } d(x_n,\partial O)$ , we have

$$ \begin{align*} \varepsilon(f^n(x))\geq e^{-\beta\varepsilon}\varepsilon(x_n),\ Q(f^n(x))\geq e^{-\gamma\varepsilon}Q(x_n). \end{align*} $$

Therefore, we obtain $e^{-\beta \varepsilon }\leq {\varepsilon (f^n(x))}/{\varepsilon (x_n)}\leq e^{\beta \varepsilon }$ and $e^{-\gamma \varepsilon }\leq {Q(f^n(x))}/{Q(x_n)}\leq e^{\gamma \varepsilon }$ if $\varepsilon>0$ is small enough. It remains to prove part (b).

First we claim that

(5.1) $$ \begin{align} \varepsilon(x_{n+1})\leq A_u^\beta e^{2\beta\varepsilon}\varepsilon(x_n), \end{align} $$

where $A_u:=[({1}/{C^u})((C^f)^{\kappa ^u}-1)+1]^{1/\gamma ^u}>1$ .

In practice, by using $e^{-\varepsilon }\leq ({d(f^n(x),\partial O)}/{d(x_n,\partial O)})\leq e^{\varepsilon }$ , equation (5.1) holds in the case $\varepsilon (f^n(x))=\varepsilon r_0^\beta $ since

$$ \begin{align*} \begin{aligned} \varepsilon(x_{n+1})&\leq\varepsilon r_0^\beta\notag\\ &\leq\varepsilon d(f^n(x),\partial O)^\beta\notag\\ &\leq\varepsilon e^{\beta\varepsilon} d(x_n,\partial O)^\beta, \end{aligned} \end{align*} $$

which implies that $\varepsilon (x_{n+1})\leq A_u^\beta e^{2\beta \varepsilon }\varepsilon (x_n)$ when $0<\varepsilon \leq A_u^\beta $ .

However, if $\varepsilon (f^n(x))=\varepsilon d(f^n(x),\partial O)^\beta $ , from Assumption US(ii) and $e^{-\varepsilon }\leq ({d(f^n(x),\partial O)}/{d(x_n,\partial O)})\leq e^{\varepsilon }$ again, we obtain for all $n\in \mathbb {Z}$ ,

$$ \begin{align*} \begin{aligned} d(x_{n+1},\partial O)&\leq e^{\varepsilon} d(f^{n+1}(x),\partial O)\notag\\ &\leq A_ue^\varepsilon d(f^n(x),\partial O)\notag\\ &\leq A_ue^{2\varepsilon} d(x_n,\partial O). \end{aligned} \end{align*} $$

Then $\varepsilon (x_{n+1})\leq A_u^\beta e^{2\beta \varepsilon }\varepsilon (x_n)$ , which completes the proof of the claim.

Denote $A:=({1}/{C})((C^f)^{\kappa }-1)+1>1$ , and according to property (a) and equation (3.5) of Lemma 3.2, we get for all $n\in \mathbb {Z}$ ,

(5.2) $$ \begin{align} Q(x_{n+1})&\leq e^{\gamma\varepsilon} Q(f^{n+1}(x))\notag\\ &\leq Ae^{\gamma\varepsilon} Q(f^n(x))\notag\\ &\leq Ae^{2\gamma\varepsilon} Q(x_n), \end{align} $$

and

(5.3) $$ \begin{align} Q(f(x_{n+1}))&\leq A Q(x_{n+1})\notag\\ &\leq A^2e^{2\gamma\varepsilon} Q(x_n)\notag\\ &\leq A^3e^{2\gamma\varepsilon} Q(f(x_n)). \end{align} $$

Combining equations (5.1), (5.2), and (5.3), we have

$$ \begin{align*} \begin{aligned} d(f^{n+1}(x),x_{n+1})&\leq r(x_{n+1})\notag\\ &\leq\varepsilon\delta^u(\varepsilon\varepsilon(x_{n+1})) Q(x_{n+1})^2Q(f(x_{n+1}))\notag\\ \end{aligned}\end{align*} $$
$$ \begin{align*} \begin{aligned} &\leq\varepsilon\delta^u(\varepsilon A_u^\beta e^{2\beta\varepsilon}\varepsilon(x_n))\cdot A^2e^{4\gamma\varepsilon}Q(x_n)^2\cdot A^3e^{2\gamma\varepsilon}Q(f(x_n))\notag\\ &=A^5 \cdot \varepsilon e^{6\gamma\varepsilon}\delta^u(A_u^\beta\cdot \varepsilon e^{2\beta\varepsilon}\varepsilon(x_n)) Q(x_n)^2Q(f(x_n)). \end{aligned} \end{align*} $$

Now we can verify the half of $x_n\rightarrow x_{n+1}$ for all $n\in \mathbb {Z}$ from the local monotonicity of $\delta ^u(\cdot )$ if $\varepsilon>0$ is small enough. In fact,

$$ \begin{align*} \begin{aligned} d(f(x_n),x_{n+1})&\leq d(f(x_n),f^{n+1}(x))+d(f^{n+1}(x),x_{n+1}) \notag\\ &\leq C^fd(x_n,f^n(x))+d(f^{n+1}(x),x_{n+1})\notag\\ &\leq\varepsilon[C^f\delta^u(\varepsilon\varepsilon(x_n))+A^5\cdot e^{6\gamma\varepsilon}\delta^u(A_u^\beta\cdot \varepsilon e^{2\beta\varepsilon}\varepsilon(x_n))]Q(x_n)^2Q(f(x_n))\notag\\ &\leq\delta^u(\varepsilon(x_n))Q(x_n)^2Q(f(x_n)), \end{aligned} \end{align*} $$

where the last inequality holds if $0<\varepsilon \leq \min \{1,{1}/{A_u^\beta e^{2\beta }},{1}/({C^f+A^5 e^{6\gamma }})\}$ .

Similarly, we can perform as above to conclude that

$$ \begin{align*} d(f^{-1}(x_{n+1}),x_n)\leq\delta^s(\varepsilon(x_{n+1}))Q(x_{n+1})^2Q(f^{-1}(x_{n+1})) \end{align*} $$

if $\varepsilon>0$ is small enough.

Therefore, $x_n\rightarrow x_{n+1}$ for all $n\in \mathbb {Z}$ when $\varepsilon>0$ is small enough. The proof is completed.

Let $\mathscr {G}=(V,E)$ be the directed graph with vertex set $V=\mathscr {A}$ and edge set $E= \{x\rightarrow y:x,y\in V\}$ , with $x\rightarrow y$ defined in Definition 4.3 for $x,y\in V$ . This is a countable directed graph. Every vertex of $\mathscr {G}$ has finite degree if $\varepsilon>0$ is small enough. In fact, for every $x\in V$ , if $y\in V$ satisfies $x\rightarrow y$ , we have

$$ \begin{align*} \begin{aligned} d(y,\partial O)&\geq d(f(x),\partial O)-d(y,f(x)) \notag\\ &\geq d(f(x),\partial O)-\frac{\varepsilon}{2} d(f(x),\partial O)\notag\\ &\geq e^{-\varepsilon} d(f(x),\partial O)\notag\\ &\geq A_ue^{-\varepsilon} d(x,\partial O), \end{aligned} \end{align*} $$

and from the discreteness of V (Proposition 5.1(1)), there are only finitely many $y\in V$ such that $x\rightarrow y$ .

We define $\Sigma :=\Sigma (\mathscr {G})$ to be the set of $\mathbb {Z}$ -indexed paths on $\mathscr {G}$ :

$$ \begin{align*} \Sigma:=\{\{x_n\}_{n\in\mathbb{Z}}\in V^{\mathbb{Z}}:x_n\rightarrow x_{n+1} \text{ for all } n\in\mathbb{Z}\}. \end{align*} $$

An element of $\Sigma $ is denoted by $\underline {x}:=\{x_n\}_{n\in \mathbb {Z}}$ . We equip $\Sigma $ with the metric $d(\underline {x},\underline {y})=\exp [-\min \{|n|:n\in \mathbb {Z}\ \text {such that}\ x_n\neq y_n\}]$ and the action of the left shift map $\sigma :\Sigma \rightarrow \Sigma , \sigma :\{x_n\}_{n\in \mathbb {Z}}\mapsto \{x_{n+1}\}_{n\in \mathbb {Z}}$ as before. Therefore, we get a TMS $(\Sigma ,\sigma )$ , it is locally compact since every vertex of $\mathscr {G}$ has finite degree.

Let $\Sigma ^{\#}$ denote the recurrent set of $\Sigma $ , defined by

$$ \begin{align*} \Sigma^{\#}:=\{\underline{x}\in\Sigma:\text{there exists } x,y\in V,&\text{there exists } n_k,m_k\uparrow\infty \text{ such that }\ x_{n_k}=x\\ \quad\text{and}\ x_{-m_k}=y \text{ for all } k\in \mathbb{Z}\}. \end{align*} $$

By the Poincaré recurrence theorem, every $\sigma $ -invariant probability measure gives $\Sigma ^{\#}$ full measure.

Definition 5.1. An $\varepsilon $ -recurrent-pointwise-pseudo-orbit (or $\varepsilon $ -rppo for short) in O is a sequence $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ .

Along an $\varepsilon $ -rppo $\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ , we can construct the local unstable and stable manifolds at $x_0$ since the pointwise dominated splitting holds for the property of recurrence. The ideas are simple. Let $\{V^{(n)}\}_{n=0}^\infty $ denote a sequence of t-manifolds at $x_0$ . We say that $V^{(n)}$ converges to a t-manifold V at $x_0$ if

$$ \begin{align*} d_{C^0}(V^{(n)},V)=\|\sigma^{(n)}-\sigma\|_{C^0}\underset{n \rightarrow \infty}{\longrightarrow}0, \end{align*} $$

where $\sigma ^{(n)}$ and $\sigma $ are the representing functions of $V^{(n)}$ and V, respectively.

Call a sequence $\underline {x}^+=\{x_n\}_{n\geq 0}$ a positive $\varepsilon $ -rppo if $x_n\rightarrow x_{n+1}$ for all $n\geq 0$ and $\{x_n\}_{n\geq 0}$ has constant subsequence. Similarly, a negative $\varepsilon $ -rppo is a sequence $\underline {x}^-=\{x_{-n}\}_{n\geq 0}$ such that $x_{-n}\rightarrow x_{-n+1}$ for all $n\geq 1$ and $\{x_{-n}\}_{n\geq 0}$ has constant subsequence.

For any $n\geq 1$ , let $V_{-n}^{u}$ be a u-admissible manifold at $x_{-n}$ . The unstable graph transform along $x_{-n} \rightarrow x_{-n+1}$ maps $V_{-n}^{u}$ to a u-admissible manifold at $x_{-n+1}$ , which we denote by $\mathscr {F}_{-n,-n+1}^u[V^u_{-n}]$ . Another application of the unstable graph transform, this time relative to $x_{-n+1} \rightarrow x_{-n+2}$ , maps $\mathscr {F}_{-n,-n+1}^u[V_{-n}]\in \mathscr {V}_{-n+1}^u$ to a u-admissible manifold at $x_{-n+2}$ , which we denote by $\mathscr {F}_{-n+1,-n+2}^u\circ \mathscr {F}_{-n,-n+1}^u[V^u_{-n}]$ . Continuing this way, we eventually reach a u-admissible manifold at $x_{0}$ which we denote by $\mathscr {F}_{-1,0}^u\circ \cdots \circ \mathscr {F}_{-n+1,-n+2}^u\circ \mathscr {F}_{-n,-n+1}^u[V^u_{-n}]$ . If this limit converges to a u-admissible manifold as $n\rightarrow \infty $ , we call it a local unstable manifold of a negative $\varepsilon $ -rppo $\underline {x}^-$ . Similarly, any s-admissible manifold $V^s_{n}$ at $x_{n}$ is mapped by n applications of a stable graph transform $\mathscr {F}^{s}$ to an s-admissible manifold $\mathscr {F}_{0,1}^s\circ \cdots \circ \mathscr {F}_{n-2,n-1}^s\circ \mathscr {F}_{n-1,n}^s[V^s_{n}]$ at $x_{0}$ . We call it a local stable manifold of a positive $\varepsilon $ -rppo $\underline {x}^+$ if this limit converges to an s-admissible manifold as $n\rightarrow \infty $ . Set

$$ \begin{align*} V^{u}(\underline{x}^-):=\lim _{n \rightarrow\infty}(\mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u})[V^u_{-n}] \end{align*} $$

and

$$ \begin{align*} V^{s}(\underline{x}^+):=\lim _{n \rightarrow \infty}(\mathscr{F}_{0,1}^{s} \circ \cdots \circ \mathscr{F}_{n-1, n}^{s})[V_{n}]. \end{align*} $$

Proposition 5.2. The following holds for all $\varepsilon>0$ small enough. Suppose $\{x_n\}_{n\in \mathbb {Z}}$ is an $\varepsilon $ -rppo, and choose arbitrary u-admissible manifolds $V_{-n}^{u}$ at $x_{-n}$ and arbitrary s-admissible manifolds $V_{n}^{s}$ at $x_{n}$ for $n\geq 0$ . Then:

  1. (1) $V^{u}(\underline {x}^-)$ is a u-admissible manifold at $x_0$ , and $V^{s}(\underline {x}^+)$ is an s-admissible manifold at $x_0$ ;

  2. (2) $f^{-1}[V^{u}(\{x_{-n}\}_{n\geq 0})] \subset V^{u}(\{x_{-n-1}\}_{n\geq 0})$ and $f[V^{s}(\{x_{n}\}_{n\geq 0})] \subset V^{s}(\{x_{n+1}\}_{n\geq 0})$ ;

  3. (3) if $y,z\in V^{u}(\underline {x}^-)$ , then for all $k\geq 0$ ,

    $$ \begin{align*} d(f^{-k}(y),f^{-k}(z))\leq8Q(x_0)\prod_{i=0}^{k-1}\|Df^{-1}|_{E^u(x_{-i})}\|^{1/2}. \end{align*} $$
    Similarly, if $y,z\in V^{s}(\underline {x}^+)$ , for all $k\geq 0$ , we have
    $$ \begin{align*} d(f^{k}(y),f^{k}(z))\leq8Q(x_0)\prod_{i=0}^{k-1}\|Df|_{E^s(x_i)}\|^{1/2}; \end{align*} $$
  4. (4) we have the following respective shadowing property along the negative and positive direction:

    $$ \begin{align*} \begin{aligned} &V^{u}(\underline{x}^-)=\{x\in\exp_{x_0}(S_{x_0}) \text{ for all } k\geq0, f^{-k}(x)\in\exp_{x_{-k}}(S_{x_{-k}})\},\\ &V^{s}(\underline{x}^+)=\{x\in\exp_{x_0}(S_{x_0}) \text{ for all } k\geq0, f^{k}(x)\in\exp_{x_{k}}(S_{x_{k}})\};\\ \end{aligned} \end{align*} $$
  5. (5) if $\{x_n\}_{n \in \mathbb {Z}}, \{y_n\}_{n \in \mathbb {Z}}\in \Sigma ^{\#}$ satisfy $x_i=y_i$ for $i=-N,\ldots , N$ , then

    $$ \begin{align*} d_{C^1}(V^{u}(\underline{x}^-), V^{u}(\underline{y}^-)) &\leq 2(N+1) \prod_{i=1}^{N}\|Df|_{E^s(x_{-i})}\|^{\delta/4},\\[3pt] d_{C^1}(V^{s}(\underline{x}^+), V^{s}(\underline{y}^+)) &\leq 2(N+1) \prod_{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|^{\delta/4}. \end{align*} $$

Remark 5.1. Unlike in [Reference Sarig22, Proposition 4.15], since the recurrence might be very slow, the convergence of $\prod _{i=1}^{N}\|Df|_{E^s(x_{-i})}\|$ or $\prod _{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|$ to zero might be very slow and hence the continuity of maps $\{x_n\}_{n \in \mathbb {Z}} \mapsto V^{u}(\underline {x}^-),V^{s}(\underline {x}^+)$ are not guaranteed by Assumptions US and R.

Proof. The proof is quite similar to the proof of [Reference Sarig22, Proposition 4.15]. We treat the case of u-admissible manifolds and s-admissible manifolds in the proof of items (1,2,4,5) and (3), respectively. By suitable modification to the proof, all the other cases are similar in its opposite direction.

(1) We divide our proof into three steps. First, we verify that if the limit exists, then it is independent of the choice of $V_{-n}^{u}$ . Since $\mathscr {F}_{-1,0}^{u} \circ \cdots \circ \mathscr {F}_{-n, -n+1}^{u}[V^u_{-n}]$ is a u-admissible manifold at $x_{0}$ , by using Proposition 4.3, for any other choice of u-admissible manifolds $W_{-n}^{u}$ at $ x_{-n}$ , we have

$$ \begin{align*} \begin{aligned} &d_{C^{0}}(\mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u}[V^u_{-n}], \mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u}[W^u_{-n}])\notag\\ &\quad\leq\prod_{i=1}^n \|Df|_{E^s(x_{-i})}\|^{1/2}d_{C^{0}}(V^u_{-n},W^u_{-n})\notag\\ &\quad\leq\prod_{i=1}^n \|Df|_{E^s(x_{-i})}\|^{1/2}\underset{n \rightarrow \infty}{\longrightarrow}0, \end{aligned} \end{align*} $$

since $d_{C^{0}}(V^u_{-n},W^u_{-n})\leq 2Q(x_{-n})<1$ if $\varepsilon>0$ is small enough and $\{x_{-n}\}_{n\geq 0}$ have constant subsequence. Thus, if the limit exists, then it is independent of $V_{-n}^{u}$ .

The next thing to do is to prove that the limit exists. For every $m>n $ , we have

$$ \begin{align*} \begin{aligned} &d_{C^{0}}(\mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u}[V^u_{-n}], \mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-m, -m+1}^{u}[V^u_{-m}])\notag\\ &\quad\leq\prod_{i=1}^n \|Df|_{E^s(x_{-i})}\|^{1/2}d_{C^{0}}(V^u_{-n},\mathscr{F}_{-n-1,-n}^{u} \circ \cdots \circ \mathscr{F}_{-m, -m+1}^{u}[V^u_{-m}])\notag\\ &\quad\leq\prod_{i=1}^n \|Df|_{E^s(x_{-i})}\|^{1/2}\underset{n \rightarrow \infty}{\longrightarrow}0. \end{aligned} \end{align*} $$

Hence, $\{\mathscr {F}_{-1,0}^{u} \circ \cdots \circ \mathscr {F}_{-n, -n+1}^{u}[V^u_{-n}]\}_{n\geq 1}$ is a Cauchy sequence and therefore converges.

Finally, we have to show the admissibility of the limit. Since $\mathscr {F}_{-1,0}^{u} \circ \cdots \circ \mathscr {F}_{-n, -n+1}^{u}[V^u_{-n}] \underset {n \rightarrow \infty }{\longrightarrow } V^{u}[\{x_{-n}\}_{n\geq 0}]$ , we have $\sigma ^{(n)} \underset {n \rightarrow \infty }{\longrightarrow } \sigma $ uniformly on $B_{x_0}^u(Q(x_0))$ , where $\sigma $ and $\sigma ^{(n)}$ represent $V^{u}[\{x_{-n}\}_{n\geq 0}]$ and $\mathscr {F}_{-1,0}^{u} \circ \cdots \circ \mathscr {F}_{-n, -n+1}^{u}[V^u_{-n}]$ , respectively.

Due to property (AM3), that is, $\operatorname {Hol}_{\delta /2}(D\sigma ^{(n)})\leq \tfrac 12$ and $\|D\sigma ^{(n)}\|_{C^0}\leq \tfrac 12$ , by the Arzelà–Ascoli theorem, $\text {there exists } n_{k} \uparrow \infty $ such that $D\sigma ^{(n_k)}\underset {k \rightarrow \infty }{\longrightarrow } \omega $ uniformly where $\|\omega \|_{C^{\delta /2}} \leq \tfrac 12$ . Thus, for any $v\in B_{x_0}^u(Q(x_0))$ ,

$$ \begin{align*}\sigma^{(n_k)}(v)=\sigma^{(n_k)}(0)+\int_0^1 D_{\unicode{x3bb} v}\sigma^{(n_k)}\cdot vd\unicode{x3bb}\underset{k \rightarrow \infty}{\longrightarrow} \sigma(0)+\int_0^1 \omega(\unicode{x3bb} v)\cdot vd\unicode{x3bb}\end{align*} $$

and hence $\sigma $ is differentiable, and $D\sigma =\omega $ . We also see that $\{D\sigma ^{(n)}\}$ can only have one limit point. Consequently, $D\sigma ^{(n)}\underset {n \rightarrow \infty }{\longrightarrow } D\sigma $ uniformly. It follows that $\|\sigma (0)\| \leq 10^{-3}Q(x_0)$ , $\|D\sigma \|_{C^0} \leq \sqrt {\varepsilon }$ , and $\|D\sigma \|_{C^{\delta /2}}\leq \tfrac 12$ ; hence the u-admissibility of $V^{u}(\underline {x}^-)$ .

(2) By the continuity of $\mathscr {F}_{-1,0}^{u}$ and the definition of $\mathscr {F}_{-1,0}^{u}$ , we have

$$ \begin{align*} \begin{aligned} V^{u}(\{x_{-n}\}_{n\geq0})&=\lim _{n \rightarrow\infty}(\mathscr{F}_{-1,0}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u})[V^u_{-n}]\notag\\ &=\mathscr{F}_{-1,0}^{u}\Big[\lim _{n \rightarrow\infty}(\mathscr{F}_{-2,-1}^{u} \circ \cdots \circ \mathscr{F}_{-n, -n+1}^{u})[V^u_{-n}]\Big]\notag\\ &=\mathscr{F}_{-1,0}^{u}[ V^{u}(\{x_{-n-1}\}_{n\geq0})]\notag\\ &\subset f[ V^{u}(\{x_{-n-1}\}_{n\geq0})]. \end{aligned} \end{align*} $$

(3) We write

$$ \begin{align*} V^{s}(\{x_{n}\}_{n\geq0})=\exp_{x_0}\{(\sigma^s_{0}(v^s_0), v^s_0):\|v^s_0\| \leq Q(x_0)\} \end{align*} $$

and

$$ \begin{align*} V^{s}(\{x_{n+k}\}_{n\geq0})=\exp_{x_k}\{(\sigma^s_k(v^s_k), v^s_k):\|v^s_k\| \leq Q(x_{k})\}\quad \text{for all } k\geq0. \end{align*} $$

Admissibility implies that $\|\sigma ^s_k(0)\| \leq 10^{-3} Q(x_k)$ and $Lip(\sigma ^s_k)\leq \sqrt {\varepsilon }$ for all $k\geq 0$ .

By part (2), $f^{k}[V^s(\{x_{n}\}_{n\geq 0})]\subset V^{s}(\{x_{n+k}\}_{n\geq 0}) \subset \exp _{x_k}(S_{x_k})$ for all $k \geq 0$ . Therefore, for any $y, z \in V^s(\{x_{n}\}_{n\geq 0})$ , one can write $f^{k}(y)=\exp _{x_{k}}(\sigma ^s_k(v^s_k), v^s_k)$ and $f^{k}(z)=\exp _{x_k}(\sigma ^s_k(w^s_k), w^s_k)$ .

For all $k \geq 0$ , since the exponential map has Lipschitz constant less than two, we get

$$ \begin{align*} \begin{aligned} d(f^{k}(y),f^{k}(z))&\leq2(\|v^s_{k}-w^s_{k}\|+\mathrm{Lip}(\sigma^s_{k})\|v^s_{k}-w^s_{k}\|)\notag\\ &\leq4\|v^s_{k}-w^s_{k}\| \end{aligned} \end{align*} $$

if $0<\varepsilon \leq 1$ .

Notice that

$$ \begin{align*} (\sigma^s_{k}(v^s_{k}), v^s_{k})&=F_{x_{k-1},x_{k}}(\sigma^s_{k-1}(v^s_{k-1}), v^s_{k-1})\quad \text{and}\quad (\sigma^s_{k}(w^s_{k}), w^s_{k})\\&=F_{x_{k-1},x_{k}}(\sigma^s_{k-1}(w^s_{k-1}), w^s_{k-1}), \end{align*} $$

or in the s-direction,

$$ \begin{align*} v^s_{k}=D^{ss}_{x_{k-1},x_{k}}(v^s_{k-1})+D^{su}_{x_{k-1},x_{k}}\circ\sigma^s_{k-1}(v^s_{k-1})+\phi^s_{x_{k-1},x_{k}}(\sigma^s_{k-1}(v^s_{k-1}), v^s_{k-1}) \end{align*} $$

and

$$ \begin{align*} w^s_{k}=D^{ss}_{x_{k-1},x_{k}}(w^s_{k-1})+D^{su}_{x_{k-1},x_{k}}\circ\sigma^s_{k-1}(w^s_{k-1})+\phi^s_{x_{k-1},x_{k}}(\sigma^s_{k-1}(w^s_{k-1}), w^s_{k-1}). \end{align*} $$

So we have

$$ \begin{align*} \begin{aligned} \tfrac{1}{4}d(f^{k}(y),f^{k}(z))&\leq\|v^s_{k}-w^s_{k}\|\notag\\ &\leq(\|D^{ss}_{x_{k-1},x_{k}}\|+\|D^{su}_{x_{k-1},x_{k}}\|+2\operatorname{Lip}(\phi^s_{x_{k-1},x_{k}}) )\|v^s_{k-1}-w^s_{k-1}\|\notag\\ &\leq\|Df|_{E^s(x_{k-1})}\|^{1/2}\|v^s_{k-1}-w^s_{k-1}\| \end{aligned} \end{align*} $$

as at the end of the proof of Proposition 4.3(1). Thus,

$$ \begin{align*} \begin{aligned} d(f^{k}(y),f^{k}(z))&\leq4\prod_{i=0}^{k-1}\|Df|_{E^s(x_i)}\|^{1/2}\|v^s_0-w^s_0\|\notag\\ &\leq8Q(x_0)\prod_{i=0}^{k-1}\|Df|_{E^s(x_i)}\|^{1/2}. \end{aligned} \end{align*} $$

(4) The inclusion $\subseteq $ is trivial. In fact, notice that $V^{u}(\underline {x}^-)$ is a u-admissible manifold at $x_0$ , it is contained in $\exp _{x_0}(S_{x_0})$ , that is, for every $x\in V^{u}(\underline {x}^-)$ , $x\in \exp _{x_0}(S_{x_0})$ . By part (2), for every $k \geq 0$ ,

$$ \begin{align*} f^{-k}(x) \in f^{-k}[V^{u}(\{x_{-n}\}_{n\geq0})] \subseteq V^{u}(\{x_{-n-k}\}_{n \geq 0}) \subset \exp_{x_{-k}}(S_{x_{-k}}) \end{align*} $$

because $V^{u}(\{x_{-n-k}\}_{n \geq 0})$ is a u-admissible manifold at $x_{-k}$ . We have $\subseteq $ .

Now we prove $\supseteq $ . An outline of the proof of this inclusion is as follows. For every point x satisfying $f^{-k}(x)\in \exp _{x_{-k}}(S_{x_{-k}})$ for all $k \geq 0$ , write $x=\exp _{x_{0}}(v^u_{0}, v^s_{0})$ . We show that $x \in V^{u}(\{x_{-n}\}_{n\geq 0})$ by proving that $v^s_{0}=\sigma ^u(v^u_{0})$ , where $\sigma ^u$ is the function which represents $V^{u}(\{x_{-n}\}_{n\geq 0})$ .

Introduce for this purpose the point $\bar {x}=\exp _{x_{0}}(\bar {v}^u_{0}, \bar {v}^s_{0})\in V^{u}(\{x_{-n}\}_{n\geq 0})$ , where $\bar {v}^u_{0}=v^u_{0}$ and $\bar {v}^s_{0}=\sigma ^u(\bar {v}^u_{0})$ . Our task now is to prove $\bar {v}^s_{0}=v^s_{0}$ .

For every $k \geq 0$ , write

$$ \begin{align*} f^{-k}(x)=\exp_{x_{-k}}(v^u_{-k}, v^s_{-k})\quad \text{and}\quad f^{-k}(\bar{x})=\exp_{x_{-k}}(\bar{v}^u_{-k}, \bar{v}^s_{-k})\in V^{u}(\{x_{-n-k}\}_{n \geq 0}), \end{align*} $$

where $\|v^u_{-k}\|,\|v^s_{-k}\|,\|\bar {v}^u_{-k}\|,\|\bar {v}^u_{-k}\| \leq Q(x_{-k})$ for all $k \geq 0$ .

By Proposition 3.1 in its version for $f^{-1}$ , for every $k \geq 0, F_{x_{-k-1}x_{-k}}^{-1}=\exp _{x_{-k-1}}^{-1} \circ f^{-1} \circ \exp _{x_{-k}}$ can be put in the form

$$ \begin{align*} \begin{aligned} &F^{-1}_{x_{-k-1},x_{-k}}(v_{-k}^u,v_{-k}^s)\notag\\ &\quad=(\bar{D}^{uu}_{x_{-k},x_{-k-1}}(v_{-k}^u)+\bar{D}^{us}_{x_{-k},x_{-k-1}}(v_{-k}^s) +\bar{\phi}^u_{x_{-k},x_{-k-1}}(v_{-k}^u,v_{-k}^s), \bar{D}^{ss}_{x_{-k},x_{-k-1}}(v_{-k}^s)\\&\qquad+\bar{D}^{su}_{x_{-k},x_{-k-1}}(v_{-k}^u)+\bar{\phi}^s_{x_{-k},x_{-k-1}}(v_{-k}^u,v_{-k}^s)) \end{aligned} \end{align*} $$

under the basis $(E^u,E^s)$ for all $v_{-k}=(v_{-k}^u,v_{-k}^s)\in S_{x_{-k}}$ , where

$$ \begin{align*}\bar{D}^{\tau t}_{x_{-k},x_{-k-1}}&=P_{x_{-k-1}}^{\tau}\circ D_{f^{-1}(x_{-k})}\exp^{-1}_{x_{-k-1}}\circ D_{x_{-k}}f^{-1}|_{E^t(x_{-k})}:B_{x_{-k}}^t(Q(x_{-k}))\\&\quad\rightarrow E^\tau(x_{-k-1}), \tau,t=u,s.\end{align*} $$

Since $d(f^{-1}(x_{-k}), x_{-k-1})<\delta ^s(\varepsilon (x_{-k}))$ , in the s-direction, we have

$$ \begin{align*}\|\bar{D}^{su}_{x_{-k},x_{-k-1}}\|\leq\varepsilon\varepsilon(x_{-k}),\end{align*} $$
$$ \begin{align*} m(D f^{-1}|_{E^{s}(x_{-k})})\leq m(\bar{D}^{ss}_{x_{-k},x_{-k-1}})+\varepsilon\varepsilon(x_{-k}).\end{align*} $$

While in the u-direction, we have

$$ \begin{align*}\|\bar{D}^{us}_{x_{-k},x_{-k-1}}\|\leq\varepsilon\varepsilon(x_{-k}),\end{align*} $$
$$ \begin{align*}\|\bar{D}^{uu}_{x_{-k},x_{-k-1}}\|\leq\|D f^{-1}|_{E^{u}(x_{-k})}\|+\varepsilon\varepsilon(x_{-k}),\end{align*} $$

and moreover,

$$ \begin{align*} \operatorname{Lip}(\bar{\phi}_{x_{-k},x_{-k-1}})\leq\varepsilon\varepsilon(x_{-k}), \end{align*} $$

where $\bar {\phi }=(\bar {\phi }^u,\bar {\phi }^s)$ .

Let $\Delta v^u_{-k}:=v^u_{-k}-\bar {v}^u_{-k}$ and $\Delta v^s_{-k}:=v^s_{-k}-\bar {v}^s_{-k}$ . Observe that for every $k \geq 0$ , $(v^u_{-k-1}, v^s_{-k-1})=F_{x_{-k-1}x_{-k}}^{-1}(v^u_{-k}, v^s_{-k})$ , and $(\bar {v}^u_{-k-1}, \bar {v}^s_{-k-1})=F_{x_{-k-1}x_{-k}}^{-1}{ }(\bar {v}^u_{-k}, \bar {v}^s_{-k})$ , we have

$$ \begin{align*} \begin{aligned} \|\Delta v^u_{-k-1}\|&\leq\|\bar{D}^{uu}_{x_{-k},x_{-k-1}}\|\cdot \|\Delta v_{-k}^u\|+\|\bar{D}^{us}_{x_{-k},x_{-k-1}}\|\cdot \|\Delta v_{-k}^s\|\\ &\quad+\operatorname{Lip}(\bar{\phi}^u_{x_{-k},x_{-k-1}})(\|\Delta v_{-k}^u\|+\|\Delta v_{-k}^s\|)\notag\\ &\leq(\|Df^{-1}|_{E^u(x_{-k})}\|+2\varepsilon\varepsilon(x_{-k}))\|\Delta v^u_{-k}\|+2\varepsilon\varepsilon(x_{-k})\|\Delta v^s_{-k}\| \notag \end{aligned} \end{align*} $$

and

$$ \begin{align*} \begin{aligned} \|\Delta v^s_{-k-1}\|&\geq m(\bar{D}^{ss}_{x_{-k},x_{-k-1}})\|\Delta v_{-k}^s\|-\|\bar{D}^{su}_{x_{-k},x_{-k-1}}\|\cdot \|\Delta v_{-k}^u\|\\ &\quad-\operatorname{Lip}(\bar{\phi}^s_{x_{-k},x_{-k-1}})(\|\Delta v_{-k}^u\|+\|\Delta v_{-k}^s\|)\notag\\ &\geq (m(Df^{-1}|_{E^s(x_{-k})})-2\varepsilon\varepsilon(x_{-k}))\|\Delta v^s_{-k}\|-2\varepsilon\varepsilon(x_{-k})\|\Delta v^u_{-k}\|. \end{aligned} \end{align*} $$

We claim that an easy induction gives $\|\Delta v^u_{-k}\|\leq \|\Delta v^s_{-k}\| \leq \|\Delta v^s_{-k-1}\|$ for all $k\geq 0$ . In fact, for $k=0$ , this is because $\|\Delta v^u_{0}\|=0$ by definition and $C\varepsilon \varepsilon (x_{-k})\leq m(Df^{-1}|_{E^s(x_{-k})})-1$ if $\varepsilon>0$ is small enough from Lemma 3.1. Assume by induction that $\|\Delta v^u_{-k}\|\leq \|\Delta v^s_{-k}\| \leq \|\Delta v^s_{-k-1}\|$ . Notice that $C\varepsilon (x_{-k})\leq 1-\|Df^{-1}|_{E^u(x_{-k})}\|$ from the case $f^{-1}$ of Lemma 3.2, and choosing a smaller $\varepsilon $ if necessary such that $\varepsilon \leq \min \{1,{C}/{4}\}$ , then we have

$$ \begin{align*} \begin{aligned} \|\Delta v^u_{-k-1}\| &\leq (\|Df^{-1}|_{E^u(x_{-k})}\|+2\varepsilon\varepsilon(x_{-k}))\|\Delta v^u_{-k}\|+2\varepsilon\varepsilon(x_{-k})\|\Delta v^s_{-k}\|\notag\\ & \leq(\|Df^{-1}|_{E^u(x_{-k})}\|+4\varepsilon\varepsilon(x_{-k}))\|\Delta v^s_{-k}\|\leq \|\Delta v^s_{-k}\| \leq \|\Delta v^s_{-k-1}\| \\ \end{aligned} \end{align*} $$

and

$$ \begin{align*} \begin{aligned} \|\Delta v^s_{-k-2}\| &\geq (m(Df^{-1}|_{E^s(x_{-k-1})})-2\varepsilon\varepsilon(x_{-k-1}))\|\Delta v^s_{-k-1}\|-2\varepsilon\varepsilon(x_{-k-1})\|\Delta v^u_{-k-1}\|\notag\\ &\geq(m(Df^{-1}|_{E^s(x_{-k-1})})-4\varepsilon\varepsilon(x_{-k-1})) \|\Delta v^s_{-k-1}\|\geq \|\Delta v^s_{-k-1}\|. \end{aligned} \end{align*} $$

Hence, the claim is verified.

We now return to the proof of this part. If we introduce a new constant

$$ \begin{align*} b:=\inf_{x\in O}\frac{m(Df^{-1}|_{E^s(x)})-m(Df^{-1}|_{E^s(x)})^{1/2}}{m(Df^{-1}|_{E^s(x)})-1}>0, \end{align*} $$

and choosing a smaller $\varepsilon $ if necessary such that $0<\varepsilon \leq ({bC}/{4})$ , then by Assumption US(iii), we see that

$$ \begin{align*} \begin{aligned} \|\Delta v^s_{-k-2}\|&\geq(m(Df^{-1}|_{E^s(x_{-k-1})})-bC\varepsilon(x_{-k-1}))\|\Delta v^s_{-k-1}\|\notag\\ &\geq m(Df^{-1}|_{E^s(x_{-k-1})})^{1/2}\|\Delta v^s_{-k-1}\|\notag \end{aligned} \end{align*} $$

for all $k\geq 0$ . Therefore, we get $\|\Delta v^s_{-k}\| \geq \prod _{i=0}^{k-1} m(Df^{-1}|_{E^s(x_{-i})})^{1/2} \|\Delta v^s_{0}\| $ and hence either $\|\Delta v^s_{0}\|=0$ or $\|\Delta v^s_{-k}\| \underset {k \rightarrow \infty }{\longrightarrow } \infty .$ However, $\|\Delta v^s_{-k}\|=\|v^s_{-k}-\bar {v}^s_{-k}\| \leq 2Q(x_{-k})<2$ , so $\|\Delta v^s_{0}\|=0 .$ Recall that $\Delta v^s_{0}=v^s_{0}-\bar {v}^s_{0}$ , we have $v^s_{0}=\bar {v}^s_{0}$ and then $v^s_0=\bar {v}^s_0=\sigma ^u(\bar {v}^u_0)=\sigma ^u(v^u_0)$ by definition. Thus, $x=\exp _{x_0}(v^u_0, \sigma ^u(v^u_0)) \in V^{u}(\{x_{-n}\}_{n\geq 0})$ .

(5) Given $n>N$ , let $V_{-n}^{u}$ be a u-admissible manifold at $x_{-n}$ and let $W_{-n}^u$ be a u-admissible manifold at $y_{-n}$ . For the sake of simplicity in notation, let $\mathscr {F}_{u}^{\ell }(V_{-n}^{u})$ (respectively $\mathscr {F}_{u}^{\ell }(W_{-n}^{u}))$ denote the result of applying $\mathscr {F}^{u}_{\cdot ,\cdot } \ell $ times to $V_{-n}^u$ using the path $x_{-n} \rightarrow \cdots \rightarrow x_{-n+\ell }$ (respectively using $y_{-n} \rightarrow \cdots \rightarrow y_{-n+\ell }$ ).

Here, $\mathscr {F}_{u}^{n-N}(V_{-n}^{u})$ and $\mathscr {F}_{u}^{n-N}(W_{-n}^{u})$ are u-admissible manifolds at $x_{-N}$ and $y_{-N}$ , respectively. Let $\sigma _{-N}, \widetilde {\sigma }_{-N}$ be their representing functions. Admissibility implies that

$$ \begin{align*} \begin{aligned} &\|\sigma_{-N}-\widetilde{\sigma}_{-N}\|_{C^0} \leq\|\sigma_{-N}\|_{C^0}+\|\widetilde{\sigma}_{-N}\|_{C^0}\leq2 Q(x_{-N})<1, \\ &\|D\sigma_{-N}-D\widetilde{\sigma}_{-N}\|_{C^0} \leq\|D\sigma_{-N}\|_{C^0}+\|D\widetilde{\sigma}_{-N}\|_{C^0}\leq2 \sqrt{\varepsilon}<1 \end{aligned} \end{align*} $$

if $\varepsilon $ is small enough.

For every $0\leq k\leq N$ , represent $\mathscr {F}_{u}^{n-k}[V_{-n}^{u}]$ and $\mathscr {F}_{u}^{n-k}[W_{-n}^{u}]$ by functions $\sigma _{-k}$ and $\widetilde {\sigma }_{-k}$ , respectively. By Proposition 4.3, we have

(5.4) $$ \begin{align} \|\sigma_{-k+1}-\widetilde{\sigma}_{-k+1}\|_{C^0} \leq \|Df|_{E^s(x_{-k})}\|^{1/2}\|\sigma_{-k}-\widetilde{\sigma}_{-k}\|_{C^0} \end{align} $$

and

(5.5) $$ \begin{align} \|D\sigma_{-k+1}-D\widetilde{\sigma}_{-k+1}\|_{C^0} \leq \|Df|_{E^s(x_{-k})}\|^{1/2}(\|D\sigma_{-k}-D\widetilde{\sigma}_{-k}\|_{C^0}+2\| \sigma_{-k}-\widetilde{\sigma}_{-k}\|_{C^0}^{\delta / 2}). \end{align} $$

Iterating equation (5.4), from $k=N$ and going down, we get

$$ \begin{align*} \begin{aligned} \|\sigma_{-k}-\widetilde{\sigma}_{-k}\|_{C^0} &\leq\|Df|_{E^s(x_{-k-1})}\|^{1/2}\|\sigma_{-k-1}-\widetilde{\sigma}_{-k-1}\|_{C^0}\notag\\ &\leq\prod^{N}_{i=k+1}\|Df|_{E^s(x_{-i})}\|^{1/2}\|\sigma_{-N}-\widetilde{\sigma}_{-N}\|_{C^0}\notag\\ &\leq\prod^{N}_{i=k+1}\|Df|_{E^s(x_{-i})}\|^{1/2}, \end{aligned} \end{align*} $$

and hence $d_{C^0}(\mathscr {F}_{u}^{n}[V_{-n}^{u}], \mathscr {F}_{u}^{n}[W_{-n}^{u}]) \leq \prod ^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2}$ . Passing to the limit ${n \rightarrow \infty }$ , we obtain

$$ \begin{align*} d_{C^0}(V^{u}(\{x_{-n}\}_{n\geq0}), V^{u}(\{y_{-n}\}_{n\geq0})) \leq \prod^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2}. \end{align*} $$

Apply $\|\sigma _{-k}-\widetilde {\sigma }_{-k}\|_{C^0} \leq \prod ^{N}_{i=k+1}\|Df|_{E^s(x_{-i})}\|^{1/2}$ to equation (5.5), and set $c_{-k}:=\|D\sigma _{-k}-D\widetilde {\sigma }_{-k}\|_{C^0}$ for every $0\leq k\leq N$ . Then $c_{-k+1} \leq \|Df|_{E^s(x_{-k})}\|^{1/2}(c_{-k}+2\prod ^{N}_{i=k+1} \|Df|_{E^s(x_{-i})}\|^{\delta /4} )$ for every $0\leq k\leq N$ . Now an easy induction gives that for every $0 \leq k \leq N$ ,

$$ \begin{align*} \begin{aligned} c_0 &\leq \prod^{k}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2} c_{-k}+2\times\bigg[\prod^{k}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2}\cdot\prod^{N}_{i=k+1}\|Df|_{E^s(x_{-i})}\|^{\delta/4}\notag\\ &\quad+\prod^{k-1}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2}\cdot\prod^{N}_{i=k}\|Df|_{E^s(x_{-i})}\|^{\delta/4} +\cdots+\|Df|_{E^s(x_{-1})}\|^{1/2}\\ &\quad\times\prod^{N}_{i=2}\|Df|_{E^s(x_{-i})}\|^{\delta/4}\bigg]. \end{aligned} \end{align*} $$

We now take $k=N$ , paying attention to the inequalities $\|Df|_{E^s(x_{-i})}\|^{1/2} \leq \|Df|_{E^s(x_{-i})}\|^{\delta /4}$ for all $i=1,\ldots ,N$ since $0<\delta <\min \{1,\alpha -{\beta }/{\gamma }\}$ and noting that $c_{-N} \leq 1$ , we have

$$ \begin{align*} c_{0} \leq \prod^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{1/2}+2 N \prod^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{\delta/4}<(2 N+1) \prod^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{\delta/4}. \end{align*} $$

Immediately, it follows that $d_{C^1}(\mathscr {F}^n_{u}[V_{-n}^{u}], \mathscr {F}^n_{u}[W^u_{-n}]) \kern1pt{\leq}\kern1pt 2(N+1) \prod ^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{\delta /4}$ . In part (1), we saw that $\mathscr {F}^n_{u}[V_{-n}^{u}]$ and $\mathscr {F}_{u}^{n}[W_{-n}^{u}]$ converge to $V^{u}(\{x_{-n}\}_{n \geq 0})$ and $V^{u}(\{y_{-n}\}_{n \geq 0})$ in $C^{1}$ , respectively. If we pass to the limit as $n \rightarrow \infty $ , finally we get

$$ \begin{align*}d_{C^1}(V^{u}(\{x_{-n}\}_{n \geq 0}), V^{u}(\{y_{-n}\}_{n \geq 0})) \leq 2(N+1) \prod^{N}_{i=1}\|Df|_{E^s(x_{-i})}\|^{\delta/4}.\\[-50pt] \end{align*} $$

We will see that Proposition 5.2 ensures that every $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ is associated to a unique point.

Definition 5.2. We say that an $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ in O shadows a point $x \in O$ when ${f^{n}(x)\in \exp _{x_n}(S_{x_n})}$ for all $n \in \mathbb {Z}$ .

The following lemma is the so called the shadowing lemma, which is at the heart in the proof of Theorem 5.1. The general idea is similar to what Sarig does in [Reference Sarig22, §4.3].

Lemma 5.1. Every $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ in O shadows a unique point $x \in O$ .

Proof. Let $\underline {x}\in \Sigma ^{\#}$ be an $\varepsilon $ -rppo. From Proposition 4.1(1), there is a singleton set ${\{x\}:=V^u(\underline {x}^-)\cap V^s(\underline {x}^+)\subset O}$ , we claim that $\underline {x}$ shadows x and $x\in O$ . By Proposition 5.2(2), for all $k\geq 0$ , we have

$$ \begin{align*} f^{-k}(x)\in f^{-k}[V^u(\{x_{-n}\}_{n\geq0})]\subset V^u(\{x_{-n-k}\}_{n\geq0})\subset\exp_{x_{-k}}(S_{x_{-k}}) \end{align*} $$

and

$$ \begin{align*} f^k(x)\in f^k[V^s(\{x_n\}_{n\geq0})]\subset V^s(\{x_{n+k}\}_{n\geq0})\subset\exp_{x_k}(S_{x_k}), \end{align*} $$

that is, $f^{k}(x)\in \exp _{x_k}(S_{x_k})$ for all $k \in \mathbb {Z}$ , and hence $\underline {x}$ shadows x.

If $y\in O$ is any other point shadowed by $\underline {x}$ , according to Definition 5.2 and Proposition 5.2(4), it must lie in $V^u(\underline {x}^-)\cap V^s(\underline {x}^+)=\{x\}$ .

For every $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ , let $\pi :\Sigma ^{\#}\rightarrow O$ be defined by

(5.6) $$ \begin{align} \{\pi(\underline{x})\}= V^u(\underline{x}^-)\cap V^s(\underline{x}^+). \end{align} $$

By the shadowing lemma in Lemma 5.1, $\pi (\underline {x})$ is the shadowed point of $\underline {x}$ , and the uniqueness guarantees that $\pi $ is well defined for every element of $\Sigma ^{\#}$ .

Here are the main properties of the triple $(\Sigma ^{\#},\sigma ,\pi )$ .

Theorem 5.1. The following hold for all $\varepsilon>0$ small enough.

  1. (1) $\pi \circ \sigma =f\circ \pi $ on $\Sigma ^{\#}$ .

  2. (2) $\pi (\Sigma ^\#)=O^{\#}$ .

  3. (3) $\pi :\Sigma ^\#\rightarrow O$ is continuous. More specifically, if $\underline {x}=\{x_n\}_{n \in \mathbb {Z}}, \underline {y}=\{y_n\}_{n \in \mathbb {Z}}\in \Sigma ^{\#}$ satisfy $x_i=y_i$ for $i=-N,\ldots , N$ , then

    $$ \begin{align*} d(\pi(\underline{x}),\pi(\underline{y})) \leq 6 \bigg[\prod_{i=1}^{N}\|Df|_{E^s(x_{-i})}\|^{1/2}+\prod_{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|^{1/2}\bigg]. \end{align*} $$

Remark 5.2. $(\Sigma ^{\#},\sigma ,\pi )$ is not a symbolic model for f, since $\pi $ is usually infinite-to-one.

Proof. (1) Notice that for all $\underline {x}\in \Sigma ^{\#}$ , from the shadowing lemma in Lemma 5.1 and Definition 5.2, we can denote $x=\pi (\underline {x})$ which satisfies $f^{n}(f\circ \pi (\underline {x}))=f^{n+1}(x)\in \exp _{x_{n+1}}(S_{x_{n+1}})$ for all $n \in \mathbb {Z}$ . However, since $\sigma (\underline {x})=\{x_{n+1}\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ , using the shadowing lemma in Lemma 5.1 again, we can denote $y=\pi \circ \sigma (\underline {x})$ which satisfies $f^{n}(\pi \circ \sigma (\underline {x}))=f^{n}(y)\in \exp _{x_{n+1}}(S_{x_{n+1}})$ for all $n \in \mathbb {Z}$ by Definition 5.2 again. From the uniqueness of the shadowing point, $y=f(x)$ , that is, $\pi \circ \sigma (\underline {x})=f\circ \pi (\underline {x})$ for all $\underline {x}\in \Sigma ^{\#}$ .

(2) First we prove $\pi (\Sigma ^\#)\supset O^{\#}$ . For every $x\in O^{\#}\subset O$ , looking closely into the proof of Proposition 5.1(2), we see that there exists a sequence $\{x_n\}_{n\in \mathbb {Z}}\in \Sigma $ that satisfies $d(f^n(x),x_n)<\varepsilon Q(x_n)$ and $d(x_n,\partial O)\geq e^{-\varepsilon }d(f^n(x),\partial O)$ for all $n\in \mathbb {Z}$ . By the definition of $O^{\#}$ , $d(x_n,\partial O)\geq e^{-\varepsilon }d(f^n(x),\partial O)$ means there exist sequences $n_k,m_k\uparrow \infty $ for which $d(x_{n_k},\partial O)$ and $d(x_{-m_k},\partial O)$ are bounded away from zero. By the discreteness of $\mathscr {A}$ (Proposition 5.1(1)), $x_n$ must repeat some symbol infinitely often in the past and (possibly a different symbol) in the future, that is, $\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ . Since $d(f^n(x),x_n)<\varepsilon Q(x_n)$ , that is, $f^n(x)\in \exp _{x_n}(T_{x_n}M(\varepsilon Q(x_n)))\subset \exp _{x_n}(S_{x_n})$ if $\varepsilon>0$ is small enough, from the uniqueness of the shadowing point, we have $x=\pi (\{x_n\}_{n\in \mathbb {Z}})\in \pi (\Sigma ^{\#})$ for all $n\in \mathbb {Z}$ . Thus, we get $\pi (\Sigma ^\#)\supset O^{\#}$ .

In the opposite direction, for every $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ , the shadowing lemma in Lemma 5.1 claims there is a unique $x\in O$ such that $x=\pi (\underline {x})$ . Since $d(f^n(x),x_n)\leq ({1}/{50})Q(x_n)\leq ({1}/{50})d(x_n,\partial O)$ from Proposition 4.1(1), we have

$$ \begin{align*} d(f^n(x),\partial O)\geq d(x_n,\partial O)-d(f^n(x),x_n)\geq \frac{49}{50}d(x_n,\partial O), \end{align*} $$

and then $x\in O^{\#}$ . Therefore, $\pi (\Sigma ^\#)\subset O^{\#}$ .

(3) Write $\{\pi (\underline {x})\}=V^u(\underline {x}^-)\cap V^s(\underline {x}^+)$ , $\{\pi (\underline {y})\}=V^u(\underline {y}^-)\cap V^s(\underline {y}^+)$ . From Propositions 4.1(2), 4.3(1), and using induction, we have

$$ \begin{align*} \begin{aligned} d(\pi(\underline{x}),\pi(\underline{y})) &\leq \frac{2}{1-\sqrt{\varepsilon}}[d_{C^0}(V^u(\underline{x}^-),V^u(\underline{y}^-))+d_{C^0}(V^s(\underline{x}^+),V^s(\underline{y}^+))]\notag\\ &\leq \frac{2}{1-\sqrt{\varepsilon}} \bigg[\prod_{i=1}^{N}\|Df|_{E^s(x_{-i})}\|^{1/2}+\prod_{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|^{1/2}\bigg]\notag\\ &\leq 6 \bigg[\prod_{i=1}^{N}\|Df|_{E^s(x_{-i})}\|^{1/2}+\prod_{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|^{1/2}\bigg] \end{aligned} \end{align*} $$

if $0<\varepsilon \leq \tfrac 19$ .

Finally, the continuity is obvious since

$$ \begin{align*} \lim_{N\rightarrow\infty}\prod_{i=1}^{N}\|Df|_{E^s(x_{-i})}\|=\lim_{N\rightarrow\infty}\prod_{i=1}^{N}\|Df^{-1}|_{E^u(x_{i})}\|=0.\\[-48pt] \end{align*} $$

6. Markov partitions and symbolic dynamics

Let $(\Sigma ,\sigma )$ be the TMS constructed in §5, and let $\pi :\Sigma ^{\#}\rightarrow O$ as defined in equation (5.6). In what follows, we use Theorem 5.1 to construct a cover of $O^{\#}$ that is locally finite and satisfies a (symbolic) Markov property.

Definition 6.1. Call $\mathscr {Z}:=\{Z(z): z \in \mathscr {A}\}$ the Markov cover, where

$$ \begin{align*} Z(z):=\{\pi(\underline{x}): \underline{x} \in \Sigma^{\#}, x_{0}=z\}. \end{align*} $$

In other words, $\mathscr {Z}$ is the family defined by the natural partition of $\Sigma ^{\#}$ into a cylinder at the zeroth position. Although every element $Z(z)$ of $\mathscr {Z}$ is a subset of the much smaller set $\exp _z(T_zM({2}/{50}Q(z)))$ (Proposition 4.1(1)), it is a cover of $O^{\#}$ since

$$ \begin{align*} \bigcup_{Z\in\mathscr{Z}}Z=\bigcup_{z\in \mathscr{A}}Z(z)=\pi(\Sigma^{\#})=O^{\#}. \end{align*} $$

Thus, $O=\bigcup _{Z\in \mathscr {Z}}Z\ \text {mod}\ \mu $ for every f-invariant probability measure $\mu $ supported on O.

Suppose $x \in Z(z) \in \mathscr {Z}$ , then $\text {there exists } \underline {x} \in \Sigma ^{\#}$ such that $x_{0}=z$ and $\pi (\underline {x})=x$ . Associated to $\underline {x}$ are two admissible manifolds at $z: V^{u}(\underline {x}^-)$ and $V^{s}(\underline {x}^+)$ . The following proposition says that these manifolds do not depend on the choice of $\underline {x}:$ if $\underline {y} \in \Sigma ^{\#}$ is another $\varepsilon $ -rppo such that $y_{0}=z$ and $\pi (\underline {y})=x$ , then

$$ \begin{align*} V^{u}(\underline{x}^-)=V^{u}(\underline{y}^-)\quad \text {and}\quad V^{s}(\underline{x}^+)=V^{s}(\underline{y}^+), \end{align*} $$

which allows us to define invariant fibers inside each $Z \in \mathscr {Z}$ (see Definition 6.4).

Proposition 6.1. For any $\underline {x},\underline {y}\in \Sigma ^{\#}$ such that $x_0=y_0$ and $\pi (\underline {x})=\pi (\underline {y})=x$ , we have

$$ \begin{align*} V^{u}(\underline{x}^-)=V^{u}(\underline{y}^-)\quad \text{and}\quad V^{s}(\underline{x}^+)=V^{s}(\underline{y}^+). \end{align*} $$

Proof. As proven in [Reference Sarig22, Proposition 6.4], we show the proposition for $V^{s}$ by dividing our proof into three claims, and leave the case of $V^{u}$ to the reader. Suppose $\varepsilon>0$ is small enough.

Claim 1. $f^{k}[ V^{s}(\underline {y}^+)] \subseteq \exp _{y_k}[B_{y_k}^u(\tfrac 18Q(y_k))\oplus B_{y_k}^s(\tfrac 18Q(y_k))]$ for all k large enough.

Proof of Claim 1

Recall that by Proposition 5.2(2), for all $k \geq 0$ , we have

$$ \begin{align*} f^{k}( V^{s}(\underline{y}^+)) \subset V^{s}(\{y_{n+k}\}_{n\geq 0})=\exp_{y_k}\{(\sigma^s_k(v^s_k), v^s_k):\|v^s_k\| \leq Q(y_{k})\}\subset\exp_{y_k}(S_{y_k}), \end{align*} $$

where $\sigma ^s_k$ is the function which represents s-admissible manifold $V^{s}(\{y_{n+k}\}_{n\geq 0})$ at $y_k$ for all $k\geq 0$ . Hence, for any $y \in V^{s}(\underline {y}^+)$ , one can write $f^{k}(y)=\exp _{y_{k}}(\sigma ^s_k(v^s_k), v^s_k)$ , $\|v^s_k\|\leq Q(y_k)$ .

Notice that $(\sigma ^s_{k}(v^s_{k}), v^s_{k})=F_{y_{k-1},y_{k}}(\sigma ^s_{k-1}(v^s_{k-1}), v^s_{k-1})$ , or in the s-direction,

$$ \begin{align*} v^s_{k}=D^{ss}_{y_{k-1},y_{k}}(v^s_{k-1})+D^{su}_{y_{k-1},y_{k}}\circ\sigma^s_{k-1}(v^s_{k-1})+\phi^s_{y_{k-1},y_{k}}(\sigma^s_{k-1}(v^s_{k-1}), v^s_{k-1}). \end{align*} $$

Using equations (4.1), (3.12), and $\|\phi ^s_{y_{k-1},y_{k}}(0,0)\|\leq \varepsilon \varepsilon (y_{k-1})Q(y_{k-1})$ , it follows that

$$ \begin{align*} \begin{aligned} \|v^s_{k}\|&\leq\|D^{ss}_{y_{k-1},y_{k}}\|\ \|v^s_{k-1}\|+\|D^{su}_{y_{k-1},y_{k}}\|\ \|\sigma_{k-1}^s(v^s_{k-1})\|+\|\phi^s_{y_{k-1},y_{k}}(0,0)\|\\&\quad+\operatorname{Lip}(\phi^s_{y_{k-1},y_{k}}) (\|\sigma_{k-1}^s(v^s_{k-1})\|+\|v^s_{k-1}\|))\notag\\ &\leq(\|Df|_{E^s(y_{k-1})}\|+4\varepsilon\varepsilon(y_{k-1}))\|v^s_{k-1}\|+2\varepsilon\varepsilon(y_{k-1})Q(y_{k-1}). \end{aligned} \end{align*} $$

We see that $\|v^s_{k}\| \leq a_{k}$ where $a_{k}$ is defined inductively by

$$ \begin{align*} a_{0}:=Q(y_{0}) \quad \text {and} \quad a_{k}=(\|Df|_{E^s(y_{k-1})}\|+4\varepsilon\varepsilon(y_{k-1}))a_{k-1}+2\varepsilon\varepsilon(y_{k-1})Q(y_{k-1}). \end{align*} $$

We claim that $a_{k}\leq \tfrac 18 Q(y_k)$ for some $k\geq 0$ . If the assertion would not hold, then ${Q(y_k) < 8 a_{k}}$ for all $k\geq 0$ , and hence $a_{k} <(\|Df|_{E^s(y_{k-1})}\|+20\varepsilon \varepsilon (y_{k-1})) a_{k-1}$ for all $k\geq 0$ , which implies that

$$ \begin{align*} a_{k}<\prod_{i=0}^{k-1}(\|Df|_{E^s(y_i)}\|+20\varepsilon\varepsilon(y_i)) a_{0}. \end{align*} $$

Fix $\kappa <\kappa _1<1$ , and introduce a new constant $c_1$ associated to $\kappa _1$ given by

$$ \begin{align*} c_1:=\inf_{x\in O}\frac{\|Df|_{E^s(x)}\|^{\kappa_1}-\|Df|_{E^s(x)}\|}{1-\|Df|_{E^s(x)}\|}>0, \end{align*} $$

then if $0<\varepsilon \leq ({c_1C}/{20})$ , we get

$$ \begin{align*} a_{k}<\prod_{i=0}^{k-1}\|Df|_{E^s(y_i)}\|^{\kappa_1} a_{0}. \end{align*} $$

Whereas by assumption, $a_{k}> \tfrac 18 Q(y_k)$ for all $k\geq 0$ . Since $y_{k-1}\rightarrow y_k$ , from Lemma 4.1 in the case $C_3=C_4=1$ , we obtain

$$ \begin{align*} \begin{aligned} Q(y_k)&> Q(y_k)-d(f(y_{k-1}),y_k)\notag\\ &\geq(\|Df|_{E^s(y_{k-1})}\|^\kappa+\varepsilon\varepsilon(y_{k-1}))Q(y_{k-1})\notag\\ &> \|Df|_{E^s(y_{k-1})}\|^\kappa Q(y_{k-1}). \end{aligned} \end{align*} $$

Therefore,

$$ \begin{align*} \begin{aligned} a_{k}> \tfrac{1}{8}Q(y_k)&>\tfrac{1}{8}\|Df|_{E^s(y_{k-1})}\|^\kappa Q(y_{k-1})\notag\\ &>\frac{1}{8}\prod_{i=0}^{k-1}\|Df|_{E^s(y_{i})}\|^\kappa a_0. \end{aligned} \end{align*} $$

Combining with the above, we have

$$ \begin{align*} \frac{1}{8}\leq \prod_{i=0}^{k-1}\|Df|_{E^s(y_{i})}\|^{\kappa_1-\kappa}\underset{k \rightarrow \infty}{\longrightarrow} 0, \end{align*} $$

which is a contradiction. Consequently, we infer that $\text {there exists } k_0\geq 0$ such that ${a_{k_0}\leq \tfrac 18Q(y_{k_0})}$ .

Moreover, we have $a_{k}\leq \tfrac 18Q(y_k)$ for all k large enough by using induction. In fact, suppose that the inequality is true for $k-1$ , we have by the definition of $a_k$ that

$$ \begin{align*} \begin{aligned} a_{k}&\leq(\|Df|_{E^s(y_{k-1})}\|+4\varepsilon\varepsilon(y_{k-1}))\tfrac{1}{8}Q(y_{k-1})+2\varepsilon\varepsilon(y_{k-1})Q(y_{k-1})\notag\\ &\leq(\|Df|_{E^s(y_{k-1})}\|+20\varepsilon\varepsilon(y_{k-1}))\tfrac{1}{8}Q(y_{k-1})\notag\\ &\leq\|Df|_{E^s(y_{k-1})}\|^{\kappa_1}\tfrac{1}{8}Q(y_{k-1})\notag\\ &\leq\|Df|_{E^s(y_{k-1})}\|^{\kappa}\tfrac{1}{8}Q(y_{k-1})\notag\\ &\leq\tfrac{1}{8}Q(y_k). \end{aligned} \end{align*} $$

Thus, $a_{k}\leq \tfrac 18Q(y_k)$ for all k large enough.

In particular, $\|v^s_k\|\leq \tfrac 18Q(y_k)$ for all k large enough. Since $\|\sigma ^s_{k}(v^s_{k})\| \leq \|\sigma ^s_{k}(0)\|+\operatorname {Lip}(\sigma ^s_{k})\|v^s_{k}\|<(10^{-3}+\sqrt {\varepsilon }) Q(y_k)\leq \tfrac 18Q(y_k)$ , if $\varepsilon $ is small enough, we have

$$ \begin{align*} f^{k}[ V^{s}(\underline{y}^+)] \subseteq \exp_{y_k}\bigg[B_{y_k}^u\bigg(\frac{1}{8}Q(y_k)\bigg)\oplus B_{y_k}^s\bigg(\frac{1}{8}Q(y_k)\bigg)\bigg] \end{align*} $$

for all k large enough.

Claim 2. $f^{k}[ V^{s}(\underline {y}^+)] \subseteq \exp _{x_k}(S_{x_k})$ for all k large enough.

Proof of Claim 2

For any $y\in V^{s}(\underline {y}^+)$ , since $\pi (\underline {x})=\pi (\underline {y})=x$ , from Proposition 4.1(1), we get

$$ \begin{align*} d(y_k,x_k)\leq d(y_k,f^k(x))+d(f^k(x),x_k)\leq \frac{1}{50}Q(y_k)+\frac{1}{50}Q(x_k), \end{align*} $$

and hence $d(f^k(y),x_k)\leq d(f^k(y),y_k)+d(y_k,x_k)<\rho (M)$ and we have $f^k(y)\in B(x_k, \rho (M))$ . Now for $k>0$ large enough, by Claim 1, we have

$$ \begin{align*} \begin{aligned} \|\!\exp_{x_k}^{-1}f^k(y)\|&\leq\|\!\exp_{y_k}^{-1}f^k(y)\|+d(y_k,x_k)\notag\\ &\leq\frac{1}{4}Q(y_k)+\frac{1}{50}Q(x_k)+\frac{1}{50}Q(y_k)\notag\\ &\leq\tfrac{1}{4}(2Q(y_k)+Q(x_k)). \end{aligned} \end{align*} $$

Note that $Q(x_k)\leq \varepsilon ^{{2}/({\alpha -\delta })}d(x_k,\partial O)$ , then

$$ \begin{align*} \begin{aligned} d(f^k(x),\partial O)&\leq d(x_k,\partial O)+d(x_k,f^k(x))\notag\\ &\leq d(x_k,\partial O)+\frac{1}{50}Q(x_k)\notag\\ &\leq e^{\varepsilon^{{2}/({\alpha-\delta})}}d(x_k,\partial O) \end{aligned} \end{align*} $$

and we have $Q(f^k(x))\leq e^{\gamma \varepsilon ^{{2}/({\alpha -\delta }})} Q(x_k)$ .

Similarly, from

$$ \begin{align*} \begin{aligned} d(f^k(x),\partial O)&\geq d(y_k,\partial O)-d(y_k,f^k(x))\notag\\ &\geq d(y_k,\partial O)-\frac{1}{50}Q(y_k)\notag\\ &\geq e^{-\varepsilon^{{2}/({\alpha-\delta})}}d(y_k,\partial O), \end{aligned} \end{align*} $$

we have $Q(f^k(x))\geq e^{-\gamma \varepsilon ^{{2}/({\alpha -\delta })}} Q(y_k)$ . Thus, we arrive at two useful inequalities:

(6.1) $$ \begin{align} d(y_k,\partial O)\leq e^{\varepsilon^{{2}/({\alpha-\delta})}}d(f^k(x),\partial O)\leq e^{2\varepsilon^{{2}/({\alpha-\delta})}}d(x_k,\partial O) \end{align} $$

and

(6.2) $$ \begin{align} Q(y_k)\leq e^{\gamma\varepsilon^{{2}/({\alpha-\delta})}}Q(f^k(x))\leq e^{2\gamma\varepsilon^{{2}/({\alpha-\delta})}}Q(x_k). \end{align} $$

This leads to

$$ \begin{align*} \begin{aligned} \|\!\exp_{x_k}^{-1}f^k(y)\|&\leq\tfrac{1}{4}(2Q(y_k)+Q(x_k))\notag\\ &\leq\tfrac{1}{4}(2e^{2\gamma\varepsilon^{{2}/({\alpha-\delta})}}+1)Q(x_k)\notag\\ &\leq Q(x_k) \end{aligned} \end{align*} $$

if k is large enough and $0<\varepsilon \leq (({\log 3-\log 2})/{2\gamma })^{({\alpha -\delta })/{2}}$ .

It is now obvious that the claim holds since we have assumed as in [Reference Chen, Hu and Zhou10] that the metric on M is taken in such a way that for any $x\in O$ , $E^u(x)$ and $E^s(x)$ are pairwise orthogonal, we thus prove

$$ \begin{align*} f^{k}[ V^{s}(\underline{y}^+)] \subseteq \exp_{x_k}(S_{x_k}) \end{align*} $$

for all k large enough.

Claim 3. $V^{s}(\underline {x}^+)=V^{s}(\underline {y}^+)$ .

Proof of Claim 3

The proof of this claim is made exactly as in [Reference Ben Ovadia6, Claim 3 on p. 102] by using Claims 1 and 2.

This completes the proof of Proposition 6.1.

Definition 6.2. Suppose $Z=Z(z)\in \mathscr {Z}$ . For any $x \in Z$ , the local unstable manifold through x is defined by $V^u(x,Z):=V^{u}(\underline {x}^-)$ for some (any) $\underline {x}=\{x_{n}\}_{n \in \mathbb {Z}} \in \Sigma ^{\#}$ such that $\pi (\underline {x})=x$ and $x_{0}=z$ . Similarly, the local stable manifold through x is defined by $V^s(x,Z):=V^{s}(\underline {x}^+)$ for some (any) $\underline {x}=\{x_{n}\}_{n \in \mathbb {Z}} \in \Sigma ^{\#}$ such that $\pi (\underline {x})=x$ and $x_{0}=z$ .

By Proposition 6.1, the definitions above do not depend on the choice of $\underline {x}$ . Since $\bigcup _{Z\in \mathscr {Z}}Z=O^{\#}$ , we only construct locally unstable/stable manifolds on $O^{\#}$ rather than O as done in [Reference Chen, Hu and Zhou10].

Theorem 6.1. For every $Z\in \mathscr {Z}$ , $|\{Z^\prime \in \mathscr {Z}: Z^\prime \cap Z\neq \varnothing \}|<\infty $ .

Proof. Fix some $Z=Z(z)\in \mathscr {Z}$ . If $Z^\prime =Z^\prime (z^\prime )$ intersects Z, then there must exist two $\varepsilon $ -rppo $\underline {x},\underline {y}\in \Sigma ^{\#}$ such that $x_0=z$ , $y_0=z^\prime $ , and $\pi (\underline {x})=\pi (\underline {y})$ . From equation (6.1), we have

$$ \begin{align*} d(z,\partial O)=d(x_0,\partial O)\leq e^{2\varepsilon^{{2}/({\alpha-\delta})}}d(y_0,\partial O)=e^{2\varepsilon^{{2}/({\alpha-\delta})}}d(z^\prime,\partial O). \end{align*} $$

It follows that $Z^\prime $ belongs to $\{Z^\prime (z^\prime ):z^\prime \in \mathscr {A}, d(z^\prime ,\partial O)\geq e^{-2\varepsilon ^{{2}/({\alpha -\delta })}}d(z,\partial O)\}$ . This set is finite because of the discreteness of $\mathscr {A}$ (Proposition 5.1(1)).

Proposition 6.2. Suppose $Z \in \mathscr {Z}$ , then for any $x, y \in Z, V^{u}(x, Z)$ and $V^{s}(y, Z)$ intersect at a unique point z, and $z \in Z$ .

Proof. It follows from Proposition 4.1(1), proved as in [Reference Sarig22, Proposition 10.5].

Definition 6.3. The Smale bracket of two points $x, y \in Z \in \mathscr {Z}$ is the unique point $[x, y]_{Z} \in V^{u}(x, Z) \cap V^{s}(y, Z)$ .

Lemma 6.1. If $x,y\in Z\in \mathscr {Z}$ , then

$$ \begin{align*} V^u([x,y]_Z,Z)=V^u(x,Z)\quad \text{and}\quad V^s([x,y]_Z,Z)=V^s(y,Z). \end{align*} $$

Proof. Write $Z=Z(z)$ where $z\in \mathscr {A}$ . There are two $\varepsilon $ -rppo $\underline {x},\underline {y}\in \Sigma ^{\#}$ such that $x_0=y_0=z$ , $\pi (\underline {x})=x, \pi (\underline {y})=y$ , and so that

$$ \begin{align*} V^u(x,Z)=V^u(\underline{x}^-)\quad \text{and}\quad V^s(y,Z)=V^s(\underline{y}^+). \end{align*} $$

It holds that $\{[x,y]_Z\}=V^u(\underline {x}^-)\cap V^s(\underline {y}^+)=\{\pi (\underline {z})\}\subset Z(z)$ , where $z_0=z$ , and

$$ \begin{align*} z_n=\begin{cases} x_n, & n \leq 0, \\ y_n, & n\geq0, \end{cases}\in\Sigma^{\#}. \end{align*} $$

By Definition 6.2,

$$ \begin{align*} V^u([x,y]_Z,Z)=V^u(\underline{z}^-)=V^u(\underline{x}^-)=V^u(x,Z) \end{align*} $$

and

$$ \begin{align*} V^s([x,y]_Z,Z)=V^s(\underline{z}^+)=V^s(\underline{y}^+)=V^s(y,Z). \\[-37pt]\end{align*} $$

Lemma 6.2. Suppose $x, y \in Z(z_{0})$ , and $f(x), f(y) \in Z(z_{1})$ . If $z_{0} \rightarrow z_{1}$ , then $f([x, y]_{Z(z_{0})})=[f(x), f(y)]_{Z(z_{1})}$ .

Despite the definition of staying in window [Reference Sarig22, Definitions 6.1 and 6.2] and the conclusion that any two local stable manifolds either coincide or are disjoint [Reference Sarig22, Proposition 6.4], which are used in the proof of Lemma 6.2 above in [Reference Sarig22, Lemma 10.7], we can still circumvent the problem just by using the weaker Proposition 6.1 above to prove the conclusion, and we will see that this conclusion is just from the Markov structure of  $\Sigma ^{\#}$ .

Proof. Compared with the proof of [Reference Sarig22, Lemma 10.7], the difference is in the proof of $f[V^s(y,Z(z_0))]\subset V^s(f(y),Z(z_1))$ and $f[V^u(x,Z(z_0))]\supset V^u(f(x),Z(z_1))$ . We give the details of the first half, the other half is proved in the same way.

Since $V^s_{z_1}:=V^s(f(y),Z(z_1))=V^s(\{x_{n+1}\}_{n\geq 0})$ for any $\{x_{n+1}\}_{n\geq 0}\in \Sigma ^{\#}$ such that $x_0=z_0$ , $x_1=z_1$ , and $\pi (\{x_{n+1}\}_{n\in \mathbb {Z}})=f(y)$ , it is an s-admissible manifold at $z_1$ . By Definition 4.4, $\mathscr {F}_{z_0,z_1}^s[V^s_{z_1}]$ is the unique s-admissible manifold at $z_0$ contained in $f^{-1}(V^s_{z_1})$ , and thus our problem reduces to prove $V^s(y,Z(z_0))=\mathscr {F}_{z_0,z_1}^s[V^s_{z_1}]$ .

According to Theorem 5.1(1) and (2), $\mathscr {F}_{z_0,z_1}^s[V^s_{z_1}]=V^s(\{x_{n}\}_{n\geq 0})$ , where $x_0=z_0$ and $\pi (\{x_{n}\}_{n\in \mathbb {Z}})=y$ since the shadowing point is unique. Notice that $V^s(y,Z(z_0))=V^s(\{y_{n}\}_{n\geq 0})$ for any $\{y_{n}\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ such that $y_0=z_0$ , and $\pi (\{y_{n}\}_{n\in \mathbb {Z}})=y$ , from Proposition 6.1, so we have $V^s(y,Z(z_0))=V^s(\{y_{n}\}_{n\geq 0})=V^s(\{x_{n}\}_{n\geq 0})=\mathscr {F}_{z_0,z_1}^s[V^s_{z_1}]$ .

Definition 6.4. For any $x\in Z\in \mathscr {Z}$ , the u-fiber of x inside Z is defined as $W^{u}(x, Z):=V^u(x,Z)\cap Z$ , and the s-fiber of x inside Z is defined as $W^{s}(x, Z):=V^s(x,Z)\cap Z$ .

Obviously, since $V^{u}(x, Z)\cap V^{s}(y, Z)\subset Z$ , Proposition 6.2 and Lemma 6.1 hold for an $u/s$ -fiber also, that is, $W^{u}(x, Z)\cap W^{s}(y, Z)=V^{u}(x, Z)\cap V^{s}(y, Z)$ , and

$$ \begin{align*} W^u([x,y]_Z,Z)=W^u(x,Z)\quad \text{and}\quad W^s([x,y]_Z,Z)=W^s(y,Z) \end{align*} $$

if $x,y\in Z\in \mathscr {Z}$ .

Proposition 6.3. Suppose $Z\in \mathscr {Z}$ . For any $x,y\in Z$ , $W^{u}(x, Z)$ and $W^{u}(y, Z)$ are either equal or they are disjoint. Similarly for $W^{s}(x, Z)$ and $W^{s}(y, Z)$ .

Proof. We prove the proposition for a u-fiber and leave the case of an s-fiber to the reader.

For any $x,y\in Z$ , assume that $W^{u}(x, Z)\cap W^{u}(y, Z)\neq \varnothing $ . Let $z\in W^{u}(x, Z)\cap W^{u}(y, Z)\subset Z$ . Since $x,z\in Z$ , $\{[x,z]_Z\}$ is well defined and equal to $W^{u}(x, Z)\cap W^{s}(z, Z)$ , notice that $z\in W^{u}(x, Z)\cap W^{s}(z, Z)$ , and thus

$$ \begin{align*} z=[x,z]_Z. \end{align*} $$

By Lemma 6.1, we have $W^{u}(z, Z)=W^{u}([x,z]_Z, Z)=W^{u}(x, Z)$ .

Similarly, $W^{u}(z, Z)=W^{u}(y, Z)$ . Hence, $W^{u}(x, Z)=W^{u}(y, Z)$ .

The following proposition states the symbolic Markov property of a $u/s$ -fiber, which also follows from the Markov structure of $\Sigma ^{\#}$ .

Proposition 6.4. If $x=\pi (\underline {x})$ where $\underline {x}=\{x_{n}\}_{n \in \mathbb {Z}} \in \Sigma ^{\#}$ , then

$$ \begin{align*} f[W^{s}(x, Z(x_{0}))] \subset W^{s}(f(x), Z(x_{1}))\quad \text{and}\quad f^{-1}[W^{u}(f(x), Z(x_{1}))] \subset W^{u}(x, Z(x_{0})). \end{align*} $$

Proof. The proof is the same as in [Reference Sarig22, Proposition 10.9]. We prove the inclusion for the s-fiber. The case of the u-fiber follows by symmetry.

By Definitions 6.4 and 6.2, $W^{s}(x, Z(x_{0})) \subset V^{s}(x, Z(x_{0})) = V^{s}(\{x_{n}\}_{n \geq 0})$ . Using Proposition 5.2(2), we have

$$ \begin{align*} f( V^{s}(\{x_{n}\}_{n \geq 0})) \subseteq V^{s}(\{x_{n+1}\}_{n \geq 0}), \end{align*} $$

the last manifold is equal to $V^{s}(f(x), Z(x_{1}))$ since $\{x_{n+1}\}_{n \geq 0}\in \Sigma ^{\#}$ satisfies $x_{0+1}=x_1$ and

$$ \begin{align*} \pi(\{x_{n+1}\}_{n \geq 0})=\pi\circ\sigma(\underline{x})=f\circ\pi(\underline{x})=f(x). \end{align*} $$

Therefore, $f[W^{s}(x, Z(x_{0}))] \subset V^{s}(f(x), Z(x_{1}))$ .

Suppose $y\in W^{s}(x, Z(x_{0}))$ . Since $y\in Z(x_{0})$ , there exists an $\varepsilon $ -rppo $\underline {y}\in \Sigma ^{\#}$ such that $y_0=x_0$ and $\pi (\underline {y})=y$ . From $y,x\in Z(x_{0})$ , we know that $\{[y,x]_{Z(x_0)}\}$ is well defined and equal to $V^u(\underline {y}^-)\cap V^s(\underline {x}^+)$ . However, $y\in V^{s}(x, Z(x_0))=V^{s}(\underline {x}^+)$ and $y=\pi (\underline {y})$ implies that $y\in V^u(\underline {y}^-)\cap V^s(\underline {x}^+)$ , and thus

$$ \begin{align*} y=[y,x]_{Z(x_0)}=\pi(\underline{z}), \end{align*} $$

where $z_0=x_0$ , and

$$ \begin{align*} z_n=\begin{cases} y_n, & n \leq 0, \\ x_n, & n\geq0, \end{cases}\in\Sigma^{\#}. \end{align*} $$

Therefore, $f(y)\in Z(x_1)$ since $\{z_{n+1}\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ satisfies $z_{0+1}=z_1=x_1$ and

$$ \begin{align*} \pi(\{z_{n+1}\}_{n \geq 0})=\pi\circ\sigma(\underline{z})=f\circ\pi(\underline{z})=f(y).\\[-35pt] \end{align*} $$

Lemma 6.3. Suppose $Z,Z^{\prime }\in \mathscr {Z}$ and $Z\cap Z^{\prime }\neq \varnothing $ .

  1. (1) If $Z=Z(z)$ and $Z^{\prime }=Z^{\prime }(z^{\prime })$ , where $z,z^{\prime }\in \mathscr {A}$ , then $Z\subset \exp _{z^{\prime }}(S_{z^{\prime }})$ .

  2. (2) For any $x\in Z\cap Z^{\prime }$ , $W^u(x,Z)\subset V^u(x,Z^{\prime })$ and $W^s(x,Z)\subset V^s(x,Z^{\prime })$ .

Proof. We follow a similar strategy in [Reference Sarig22, Lemma 10.10].

(1) Note that by Proposition 4.1(1),

$$ \begin{align*} \begin{aligned} Z(z)\subset\exp_z\bigg(T_zM\bigg(\frac{2}{50}Q(z)\bigg)\bigg)\subset B\bigg(z,\frac{4}{50}Q(z)\bigg)\subset B\bigg(z^{\prime},\frac{4}{50}Q(z)+d(z,z^{\prime})\bigg). \end{aligned} \end{align*} $$

Fix some $x\in Z\cap Z^\prime \subset O$ , so from equation (6.2), we have

$$ \begin{align*} Q(z)\leq e^{2\gamma\varepsilon^{{2}/({\alpha-\delta})}}Q(z^{\prime}) \end{align*} $$

and

$$ \begin{align*} \begin{aligned} \frac{4}{50}Q(z)+d(z,z')&\leq\frac{5}{50}Q(z)+\frac{1}{50}Q(z^{\prime})\notag\\ &\leq\bigg(\frac{5}{50}e^{2\gamma\varepsilon^{{2}/({\alpha-\delta})}}+\frac{1}{50}\bigg)Q(z^{\prime})\notag\\ &\leq\frac{16}{50}Q(z^{\prime}) \end{aligned} \end{align*} $$

if $0<\varepsilon \leq ({\log 3}/{2\gamma })^{({\alpha -\delta })/{2}}$ .

Therefore,

$$ \begin{align*} Z(z)\subset B\bigg(z^{\prime},\frac{4}{50}Q(z)+d(z,z^{\prime})\bigg)\subset B\bigg(z^{\prime},\frac{8}{25}Q(z^{\prime})\bigg)\subset\exp_{z^{\prime}}(S_{z^{\prime}}). \end{align*} $$

(2) We show that $W^{s}(x, Z) \subset V^{s}(x, Z^{\prime })$ . The case of the u-direction follows by symmetry.

Since $x\in Z(z)\cap Z^\prime (z^\prime )$ , we can write $x=\pi (\underline {x})$ where $\underline {x}\in \Sigma ^{\#}$ , $x_0=z$ , and $x=\pi (\underline {y})$ , where $\underline {y}\in \Sigma ^{\#}$ , $y_0=z^\prime $ . Observe that for all $k\in \mathbb {Z}$ , $f^{k}(x)=f^k(\pi (\underline {x}))=\pi (\sigma ^k(\underline {x}))\in Z(x_{k})$ , we have $f^{k}(x)\in Z(x_{k})$ . Similarly, since $f^{k}(x)=f^k(\pi (\underline {y}))=\pi (\sigma ^k(\underline {y}))\in Z^\prime (y_{k})$ , we have $f^{k}(x)\in Z^\prime (y_{k})$ , and hence $f^{k}(x)\in Z(x_{k})\cap Z^\prime (y_{k})$ . By the first part of the lemma, $Z(x_{k}) \subset \exp _{y_{k}}(S_{y_k})$ .

Since $x=\pi (\underline {x})$ and $Z(z)=Z(x_0)$ , we have by the symbolic Markov property of an s-fiber iterated forward k times

$$ \begin{align*} f^{k}[W^{s}(x, Z(z))] \subset W^{s}(f^{k}(x), Z(x_{k}))\subset Z(x_{k}) \subset \exp_{y_{k}}(S_{y_k}) \end{align*} $$

for all $k \geq 0$ . By Proposition 5.2(4), $W^{s}(x, Z) \subset V^{s}(\underline {y}^+) = V^{s}(x, Z^{\prime })$ .

The next step to do in the construction of a Markov partition is to refine $\mathscr {Z}$ to destroy its non-trivial intersections. The result will be a partition of $O^{\#}$ by sets with the (geometrical) Markov property. This method is the so called Bowen–Sinai refinement procedure, first developed by Sinai and Bowen for finite covers [Reference Bowen8, Reference Sinai23, Reference Sinai24], and also works for countable covers satisfying the local finiteness property [Reference Sarig22, §11].

Write $\mathscr {Z}=\{Z_1,Z_2,\ldots \}$ . Following [Reference Bowen8, Reference Sarig22], we define a partition of $Z_{i}$ such that for every $Z_{i}, Z_{j} \in \mathscr {Z}$ ,

$$ \begin{align*} \begin{aligned} T_{i j}^{u s} &:=\{x \in Z_{i}: W^{u}(x, Z_{i}) \cap Z_{j} \neq \varnothing, W^{s}(x, Z_{i}) \cap Z_{j} \neq \varnothing\}, \\ T_{i j}^{u \varnothing}&: =\{x \in Z_{i}: W^{u}(x, Z_{i}) \cap Z_{j} \neq \varnothing, W^{s}(x, Z_{i}) \cap Z_{j}=\varnothing\}, \\ T_{i j}^{\varnothing s}&: =\{x \in Z_{i}: W^{u}(x, Z_{i}) \cap Z_{j}=\varnothing, W^{s}(x, Z_{i}) \cap Z_{j} \neq \varnothing\}, \\ T_{i j}^{\varnothing \varnothing}&: =\{x \in Z_{i}: W^{u}(x, Z_{i}) \cap Z_{j}=\varnothing, W^{s}(x, Z_{i}) \cap Z_{j}=\varnothing\}. \end{aligned} \end{align*} $$

Let $\mathscr {T}:=\{T_{i j}^{\alpha \beta }: i, j \in \mathbb {N}, Z_{i} \cap Z_{j} \neq \varnothing , \alpha \in \{u, \varnothing \}, \beta \in \{s, \varnothing \}\}$ .

Clearly, $T_{i i}^{u s}=Z_{i}$ ; therefore, $\mathscr {T}$ covers the same set as $\mathscr {Z}$ , namely $\pi (\Sigma ^{\#})=O^{\#}$ . Using Proposition 6.3 and Lemma 6.3(2) above, we prove that $T_{i j}^{u s}=Z_{i} \cap Z_{j}$ as in [Reference Sarig22, p. 386].

Definition 6.5. For every $x\in \pi (\Sigma ^{\#})=O^{\#}$ , let $R(x):=\underset {{\substack {T \in \mathscr {T} \\ x\in T}}}{\bigcap T}$ and set $\mathscr {R}:=\{R(x): x\in O^{\#}\}$ .

Proposition 6.5. $\mathscr {R}$ is a countable pairwise disjoint cover of $O^{\#}$ .

An outline of the proof of this proposition is as follows, the details of which we omit. Proceeding as in [Reference Sarig22, Proposition 11.2], first, from the locally finite property of $\mathscr {Z}$ (Theorem 6.1), $R(x)$ is a finite intersection of elements of $\mathscr {T}$ , that is, for every $R\in \mathscr {R}$ , $|\{Z\in \mathscr {Z}:Z\supset R\}|<\infty $ . Second, since $\mathscr {T}$ is countable and the fact that $T_{i i}^{u s}=Z_{i}$ , we conclude that $\mathscr {R}$ is a countable cover of $O^{\#}$ , that is, $\underset {R\in \mathscr {R}}\bigcup R=O^{\#}$ . Moreover, it is a countable pairwise disjoint cover of $O^{\#}$ . The key point to destroy the non-trivial intersection is to prove that $R(x)$ is the equivalence class of x for the following equivalence relation on $O^{\#}$ : for every $x, y\in O^{\#}$ , define

$$ \begin{align*} x \sim y \text { if and only if } \text{ for all } Z, Z^{\prime} \in \mathscr{Z}, \quad\left(\begin{array}{@{}rll@{}} x \in Z & \Leftrightarrow & y \in Z, \\ W^{u}(x, Z) \cap Z^{\prime} \neq \varnothing & \Leftrightarrow & W^{u}(y, Z) \cap Z^{\prime} \neq \varnothing, \\ W^{s}(x, Z) \cap Z^{\prime} \neq \varnothing & \Leftrightarrow & W^{s}(y, Z) \cap Z^{\prime} \neq \varnothing \end{array}\right)\!. \end{align*} $$

So for every $x, y \in \underset {R\in \mathscr {R}}\bigcup R=O^{\#}$ , either $R(x)=R(y)$ or $R(x) \cap R(y)=\varnothing $ . Thus, $\mathscr {R}$ is a Bowen–Sinai refinement of $\mathscr {Z}$ . For more details, see [Reference Sarig22, Proposition 11.2].

By Definition 6.5 and the local finiteness property of $\mathscr {Z}$ , the following inclusion relation and local finiteness properties for $\mathscr {R}$ are proved exactly as in [Reference Sarig22, Lemma 11.3].

Lemma 6.4. $\mathscr {R}$ is a locally finite refinement of $\mathscr {Z}$ :

  1. (1) for every $R \in \mathscr {R}$ and $Z\in \mathscr {Z}$ , if $R\cap Z\neq \varnothing $ , then $R\subset Z$ ;

  2. (2) for every $Z \in \mathscr {Z}, |\{R \in \mathscr {R}: R \subset Z\}|<\infty $ ;

  3. (3) for every $R\in \mathscr {R}$ , $|\{Z\in \mathscr {Z}:Z\supset R\}|<\infty $ .

Now we follow [Reference Sarig22, §11] to show that $\mathscr {R}$ is a Markov partition in the sense of Sinai [Reference Sinai24].

Definition 6.6. For any $R \in \mathscr {R}$ and $x\in R$ , we define the u-fiber and s-fiber of $x \textit {inside }R$ respectively by

$$ \begin{align*} W^{u}(x, R):=\bigcap_{\substack{ T_{i j}^{\alpha \beta} \in \mathscr{T} \\ T_{i j}^{\alpha \beta} \supset R}} W^{u}(x, Z_{i}) \cap T_{i j}^{\alpha \beta}\quad \text{and}\quad W^{s}(x, R):=\bigcap_{\substack{T_{i j}^{\alpha \beta} \in \mathscr{T} \\ T_{i j}^{\alpha \beta} \supset R}} W^{s}(x, Z_{i}) \cap T_{i j}^{\alpha \beta}. \end{align*} $$

Proposition 6.3 implies that any two u-fibers (s-fibers) either coincide or are disjoint: suppose $R \in \mathscr {R}$ and $x,y\in R$ , either $W^{u}(x, R)$ , $W^{u}(y, R)$ are equal or they are disjoint, and similarly for $W^{s}(x, R)$ and $W^{s}(y, R)$ . The proof is straightforward as in [Reference Sarig22, Proposition 11.5(2)].

Proposition 6.6. Suppose $R \in \mathscr {R}$ and $x,y\in R$ .

  1. (1) $W^u(x,R),W^s(x, R)\subset R$ and $W^u(x,R)\cap W^s(x, R)={x}$ .

  2. (2) The intersection $W^{u}(x, R) \cap W^{s}(y, R)$ consists of a single point and this point belongs to R. Denote it by $[x, y]_{R}$ and call the Smale bracket of $x,y$ in R.

  3. (3) Markov property: let $R_{0}, R_{1} \in \mathscr {R}$ . If $x \in R_{0}$ and $f(x) \in R_{1}$ , then

    $$ \begin{align*} f(W^{s}(x, R_{0})) \subset W^{s}(f(x), R_{1}) \quad\text{and}\quad f^{-1}(W^{u}(f(x), R_{1})) \subset W^{u}(x, R_{0}). \end{align*} $$

Proof. Part (1) is proved exactly as in [Reference Sarig22, Proposition 11.5(1)]. Using Proposition 6.3, part (2) is a standard result which can be found in [Reference Sarig22, Proposition 11.5(3)]. Along the proof, we also obtain that $[x, y]_{R}=[x, y]_{Z}$ for every $x,y\in R$ and all $Z\in \mathscr {Z}$ containing R. Finally, part (3) is the heart to obtain a Markov partition which is proved as in [Reference Sarig22, Proposition 11.7], using Propositions 6.3, 6.4, and Lemmas 6.2, 6.3(2), and the equality $[x, y]_{R}=[x, y]_{Z}$ holds for every $x,y\in R$ and every $Z\in \mathscr {Z}$ containing R.

We now construct a new symbolic coding of f, which is a symbolic model of f generated by the Markov partition $\mathscr {R}$ that satisfies Theorem 2.1. Let $\widehat {\mathscr {G}}=(\widehat {V}, \widehat {E})$ be the directed graph with vertex set $\widehat {V}=\mathscr {R}$ and edge set $\widehat {E}=\{R_1 \rightarrow R_2: R_1, R_2 \in \mathscr {R}$ such that ${R_1 \cap f^{-1}R_2 \neq \varnothing \}}$ . This is also a countable directed graph, and every vertex has finite degree because for every $R_0\in \mathscr {R}$ , if $R_1\in \mathscr {R}$ satisfies $R_0\rightarrow R_1$ , by Definition 6.5 and the local finiteness property (Lemma 6.4(3)) for $\mathscr {R}$ , there are finite points of $\mathscr {A}$ , say z such that ${R_0\subset Z(z)}$ . Since $R_0\rightarrow R_1$ , we can take $x\in R_0\cap f^{-1}(R_1)\subset Z(z)$ , there exist by Definition 6.1 an $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ such that $x_0=z$ and $\pi (\underline {x})=x$ . Then $f(x)\in R_1\cap Z(x_1)$ and from the inclusion relation (Lemma 6.4(1)) for $\mathscr {R}$ , $R_1\subset Z(x_1)$ and such $R_1$ is finite (Lemma 6.4(2)) since $Z(x_1)$ is finite for fixed $R_0$ (Lemma 6.4(3)). Therefore,

$$ \begin{align*} |\{R_1\in\mathscr{R}:R_0\rightarrow R_1\}|\leq\underset{{\substack{z\in\mathscr{A} \\ Z(z)\supset R_0}}}\sum\underset{{\substack{z^\prime\in\mathscr{A} \\ z\rightarrow z^{\prime}}}}\sum|\{R_1\in\mathscr{R}:R_1\subset Z(z^\prime)\}|<\infty. \end{align*} $$

Let $(\widehat {\Sigma }, \widehat {\sigma })$ be the TMS induced by $\widehat {\mathscr {G}}$ :

$$ \begin{align*} \widehat{\Sigma}:=\{\{R_n\}_{n\in\mathbb{Z}}\in\mathscr{R}^{\mathbb{Z}}: R_n\rightarrow R_{n+1} \text{ for all } n\in\mathbb{Z}\},\end{align*} $$

where the $\widehat {\sigma }$ is the left shift and the element of $\widehat {\Sigma }$ is denoted by $\underline {R}:=\{R_n\}_{n\in \mathbb {Z}}$ . We equip $\widehat {\Sigma }$ with the metric $d(\underline {R},\underline {S}) = \exp [-\min \{|n| : n\in \mathbb {Z}\ \text {such that}\ R_n\neq S_n\}]$ as before. Since every vertex of $\widehat {\mathscr {G}}$ has finite degree, $\widehat {\Sigma }$ is locally compact. Define as before

$$ \begin{align*} {\widehat{\Sigma}}^{\#}:=\{\underline{R}\in \widehat{\Sigma}: &\text{ there exists } R,S\in \mathscr{R}, \text{there exists } n_k,m_k\uparrow\infty \\& \text{ such that}\ R_{n_k}=R\ \text{and}\ R_{-m_k}=S \text{ for all } k\in \mathbb{Z}\}. \end{align*} $$

Again by the Poincaré recurrence theorem, every $\widehat {\sigma }-$ invariant probability measure gives $\widehat {\Sigma }^{\#}$ full measure. Furthermore, every periodic point of $\widehat {\sigma }$ is in ${\widehat {\Sigma }}^{\#}$ .

For $n \in \mathbb {Z}$ and a path $R_{-n} \rightarrow \cdots \rightarrow R_{n}$ on $\widehat {\mathscr {G}}$ , $\bigcap _{i=-n}^{n}f^{-i}(R_i) \neq \varnothing $ . This follows by induction, using the Markov property of $\mathscr {R}$ (Proposition 6.6(3)), as done originally by Adler, Weiss, and Sinai [Reference Adler and Weiss1, Reference Adler and Weiss3, Reference Sinai23, Reference Sinai24]. For more details, see [Reference Sarig22, Lemma 12.1].

Lemma 6.5. For every finite path $R_{-n} \rightarrow \cdots \rightarrow R_{n}$ on $\widehat {\mathscr {G}}$ , there exists an $\varepsilon $ -rppo $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ such that for every $i=-n,\ldots ,n$ , $R_i\subset Z(x_i)$ , and

$$ \begin{align*} \mathrm{diam}\bigg(\bigcap_{i=-n}^{n}f^{-i}(R_i)\kern-1.2pt\bigg)\kern-1.2pt\leq 8Q(x_n)\prod_{j=1}^{n}\|Df^{-1}|_{E^u(x_{j})}\|^{1/2}+8Q(x_{-n})\kern-1pt\prod_{j=1}^{n}\|Df|_{E^s(x_{-j})}\|^{1/2}. \end{align*} $$

Moreover, for every $\underline {R}=\{R_n\}_{n\in \mathbb {Z}}\in {\widehat {\Sigma }}^{\#}$ , we have

$$ \begin{align*} \mathrm{diam}\bigg(\bigcap_{i=-N}^{N}f^{-i}(R_i)\bigg)\underset{N \rightarrow \infty}{\longrightarrow}0. \end{align*} $$

Proof. Fix $x,y\in \bigcap _{i=-n}^{n}f^{-i}(R_i)$ . By Definition 6.5, we can pick some $z\in \mathscr {A}$ such that $R_0\subset Z(z)\in \mathscr {Z}$ . Since $x\in R_0\subset Z(z)$ , there exists by Definition 6.1 an $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ such that $x_0=z$ , $\pi (\underline {x})=x$ . From $f^i(x)=f^i\circ \pi (\underline {x})=\pi \circ \sigma ^i(\underline {x})\in Z(x_i)$ and $f^i(x)\in R_i$ , we have $f^i(x)\in R_i\cap Z(x_i)$ for all $i=-n,\ldots ,n$ . So we have $R_i\subset Z(x_i)$ by inclusion relation Lemma 6.4(1) for all $i=-n,\ldots ,n$ . It follows that

$$ \begin{align*} \bigcap_{i=-n}^{n}f^{-i}(R_i)\subset \bigcap_{i=-n}^{n}f^{-i}[Z(x_i)], \end{align*} $$

and hence $y\in \bigcap _{i=-n}^{n}f^{-i}[Z(x_i)]\subset Z(x_0)$ .

Since $x,y\in Z(x_0)$ , we can let $z^\prime :=[x,y]_{Z(x_0)}\in Z(x_0)$ . Notice that $f^i(x), f^i(y)\in Z(x_i)$ for all $i=-n,\ldots ,n$ and $x_0\rightarrow \cdots \rightarrow x_n$ , we have by Lemma 6.2 iterated forward n times

$$ \begin{align*} \begin{aligned} f^n(z^\prime)&=f^n([x,y]_{Z(x_0)})\notag\\ &=f^{n-1}([f(x),f(y)]_{Z(x_1)})\notag\\ &=\cdots=[f^n(x),f^n(y)]_{Z(x_n)}\notag\\ &=V^u(f^n(x),Z(x_n))\cap V^s(f^n(y),Z(x_n)), \end{aligned} \end{align*} $$

and thus $f^n(z^\prime )\in V^u(f^n(x),Z(x_n))=V^u(\{x_{-k+n}\}_{k\geq 0})$ .

Similarly, since $x_{-n}\rightarrow \cdots \rightarrow x_0$ , we have by Lemma 6.2 iterated backward n times

$$ \begin{align*} \begin{aligned} f^{-n}(z^\prime)&=f^{-n}([x,y]_{Z(x_0)})\notag\\ &=f^{-n+1}([f^{-1}(x),f^{-1}(y)]_{Z(x_{-1})})\notag\\ &=\cdots=[f^{-n}(x),f^{-n}(y)]_{Z(x_{-n})}\notag\\ &=V^u(f^{-n}(x),Z(x_{-n}))\cap V^s(f^{-n}(y),Z(x_{-n})), \end{aligned} \end{align*} $$

and thus $f^{-n}(z^\prime )\in V^s(f^{-n}(y),Z(x_{-n}))=V^s(\{x_{k-n}\}_{k\geq 0})$ .

Now using Proposition 5.2(3), for $x,y\in \bigcap _{i=-n}^{n}f^{-i}(R_i)$ , we have

$$ \begin{align*} \begin{aligned} d(x,y)&\leq d(x,z^\prime)+d(z^\prime,y)\notag\\ &=d(f^{-n}(f^n(x)),f^{-n}(f^n(z^\prime)))+d(f^{n}(f^{-n}(z^\prime)),f^{n}(f^{-n}(y)))\notag\\ &\leq 8Q(x_n)\prod_{i=0}^{n-1}\|Df^{-1}|_{E^u(x_{-i+n})}\|^{1/2}+8Q(x_{-n})\prod_{i=0}^{n-1}\|Df|_{E^s(x_{i-n})}\|^{1/2}\notag\\ &= 8Q(x_n)\prod_{j=1}^{n}\|Df^{-1}|_{E^u(x_{j})}\|^{1/2}+8Q(x_{-n})\prod_{j=1}^{n}\|Df|_{E^s(x_{-j})}\|^{1/2}. \end{aligned} \end{align*} $$

Therefore, for every finite path $R_{-n} \rightarrow \cdots \rightarrow R_{n}$ on $\widehat {\mathscr {G}}$ , there exists an $\varepsilon $ -rppo $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}$ such that

$$ \begin{align*} \mathrm{diam}\bigg(\bigcap_{i=-n}^{n}f^{-i}(R_i)\kern-1pt\bigg)\kern-1.3pt\leq8Q(x_n)\prod_{j=1}^{n}\|Df^{-1}|_{E^u(x_{j})}\|^{1/2}+8Q(x_{-n})\prod_{j=1}^{n}\|Df|_{E^s(x_{-j})}\|^{1/2}. \end{align*} $$

Finally, if $\underline {R}=\{R_n\}_{n\in \mathbb {Z}}\in {\widehat {\Sigma }}^{\#}$ , then $\text {there exists } R\in \mathscr {R}$ , such that $R_m=R$ for infinitely many $m>0$ . From Lemma 6.4(3), for this R, $|\{Z\in \mathscr {Z}:Z\supset R\}|$ is finite, so by the pigeonhole principle, $\text {there exists } \bar {x}\in \mathscr {A}$ , such that $x_m=\bar {x}$ for infinitely many $m>0$ . Similarly, $\text {there exists } \bar {y}\in \mathscr {A}$ , such that $x_m=\bar {y}$ for infinitely many $m<0$ . Thus, for every $\underline {R}\in {\widehat {\Sigma }}^{\#}$ , there exists an $\varepsilon $ -rppo $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}$ such that

$$ \begin{align*} \mathrm{diam}\bigg(\bigcap_{i=-N}^{N}f^{-i}(R_i)\bigg)\leq8Q(x_N)\prod_{j=1}^{N}\|Df^{-1}|_{E^u(x_{j})}\|^{1/2}+8Q(x_{-N})\prod_{j=1}^{N}\|Df|_{E^s(x_{-j})}\|^{1/2} \end{align*} $$

holds for every $N\geq 1$ . So we have

$$ \begin{align*} \mathrm{diam}\bigg(\bigcap_{i=-N}^{N}f^{-i}(R_i)\bigg)\underset{N \rightarrow \infty}{\longrightarrow}0.\\[-46pt] \end{align*} $$

For every $\underline {R}\in \widehat {\Sigma }^{\#}$ , let $\widehat {\pi }: \widehat {\Sigma }^{\#}\rightarrow O$ be defined by

$$ \begin{align*} \{\widehat{\pi}(\underline{R})\}:=\bigcap_{n \geq 0} \overline{\bigcap_{i=-n}^{n}f^{-i}(R_i)}. \end{align*} $$

Here, $\widehat {\pi }$ is well defined because $\overline {\bigcap _{i=-n}^{n}f^{-i}(R_i)}$ is a non-empty compact subset of M whose diameters tend to zero as $n\rightarrow \infty $ and the intersection $\bigcap _{n \geq 0} \overline {\bigcap _{i=-n}^{n}f^{-i}(R_i)}$ is a singleton.

It is worthy to point out that we take the closures of $\bigcap _{i=-n}^{n}f^{-i}(R_i)$ because the $R_i$ terms are not necessarily closed. A priori, the image of $\widehat {\pi }$ on ${\widehat {\Sigma }}^{\#}$ could be bigger than $\pi (\Sigma ^{\#})=O^{\#}$ . Fortunately, this is not the case for Theorem 2.1(3), or see the proof of the following Theorem 6.2(3).

The triple $(\widehat {\Sigma }^{\#}, \widehat {\sigma }, \widehat {\pi })$ is the one that satisfies Theorem 2.1, where the non-injectivity of $\widehat {\pi }$ is analyzed using the following notion of affiliation, which was introduced by Sarig [Reference Sarig22, §12.3].

Definition 6.7. $R,R^\prime \in \mathscr {R}$ are called affiliated if there exist $Z,Z^\prime \in \mathscr {Z}$ such that $Z\supset R$ , $Z^\prime \supset R^\prime $ , and $Z\cap Z^\prime \neq \varnothing $ . If this occurs, we write $R\sim R^\prime $ .

For $R\in \mathscr {R}$ , define $N(R):=\{(R^\prime , z)\in \mathscr {R}\times \mathscr {A}:R^\prime \sim R\ \text {and}\ Z(z)\supset R^\prime \}$ . By the local-finiteness of $\mathscr {Z}$ , and Lemma 6.4(2) and (3), $N(R)$ is finite. See the proof of [Reference Sarig22, Lemma 12.7].

Definition 6.8. We say that $\underline {R}\approx \underline {R}^\prime $ if $R_n\sim R_n^\prime $ for all $n\in \mathbb {Z}$ .

Lemma 6.6. If $\underline {R},\underline {R}^\prime \in {\widehat {\Sigma }}^{\#}$ and $\widehat {\pi }(\underline {R})=\widehat {\pi }(\underline {R}^\prime )$ , then $\underline {R}\approx \underline {R}^\prime $ .

Proof. Suppose $\underline {R}=\{R_n\}_{n\in \mathbb {Z}}\in {\widehat {\Sigma }}^{\#}$ . By Definition 6.5, we can pick some $x_0\in \mathscr {A}$ such that $R_0\subset Z(x_0)\in \mathscr {Z}$ . Since $R_0\rightarrow R_1$ , there exists a point $x\in R_0\cap f^{-1}(R_1)\subset Z(x_0)$ . So there exists by Definition 6.1 an $\varepsilon $ -rppo $\underline {x}^{\prime }\in \Sigma ^{\#}$ such that $x_0^\prime =x_0$ , $\pi (\underline {x}^{\prime })=x$ . Then $f(x)\in R_1\cap Z(x_1^\prime )$ . From Lemma 6.4(1), we have $R_1\subset Z(x_1^\prime )$ . Set $x_1=x_1^\prime $ , so we get $x_0\rightarrow x_1$ . Inductively forwards, one can proceed this construction to give us a path $x_0\rightarrow \cdots \rightarrow x_n$ on $\Sigma $ satisfies $R_n\subset Z(x_n)$ for every $n\geq 0$ . Similarly, repeating the procedure inductively backwards gives us another path $x_{-n}\rightarrow \cdots \rightarrow x_0$ on $\Sigma $ satisfies $R_{-n}\subset Z(x_{-n})$ for every $n\geq 0$ . Therefore, this procedure gives us a sequence ${\{x_n\}_{n\in \mathbb {Z}}\in \Sigma} $ . We claim that $\{x_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ for $\underline {R}\in {\widehat {\Sigma }}^{\#}$ .

In fact, since $\underline {R}\in {\widehat {\Sigma }}^{\#}$ , $\text {there exists } R\in \mathscr {R}$ , such that $R_m=R$ for infinitely many ${m>0}$ . From Lemma 6.4(3), for this R, $|\{Z\in \mathscr {Z}:Z\supset R\}|$ is finite, so by the pigeonhole principle, $\text {there exists } z\in \mathscr {A}$ , such that $x_m=z$ for infinitely many $m>0$ . Similarly, $\text { there exists } z^\prime \in \mathscr {A}$ , such that $x_m=z^\prime $ for infinitely many $m<0$ . Thus, we construct an $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ for $\underline {R}\in {\widehat {\Sigma }}^{\#}$ such that

$$ \begin{align*} z:=\widehat{\pi}(\underline{R})\in\bigcap_{n \geq 0} \overline{\bigcap_{i=-n}^{n}f^{-i}(Z(x_i))}, \end{align*} $$

that is, $f^n(z)\in \overline {Z(x_n)}$ for all $n\in \mathbb {Z}$ .

Recall that every element $Z(x_n)$ is a subset of the much smaller set $\exp _{x_n}(T_{x_n}M({2}/{50} Q(x_n)))$ (Proposition 4.1(1)), we have $d(f^n(z),x_n)\leq \mathrm {diam}(\overline {Z(x_n)})=\mathrm {diam}(Z(x_n))\leq \tfrac 12Q(x_n)$ and then $f^{n}(z)\in \exp _{x_n}(S_{x_n})$ for all $n \in \mathbb {Z}$ . By Definition 5.2 and the shadowing lemma (Lemma 5.1), $\pi (\underline {x})=z=\widehat {\pi }(\underline {R})$ .

Analogously, for $\underline {R}^\prime \in {\widehat {\Sigma }}^{\#}$ , there exist $\{y_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ such that $\pi (\underline {y})=\widehat {\pi }(\underline {R})$ . Since $\widehat {\pi }(\underline {R})=\widehat {\pi }(\underline {R}^\prime )=z$ , we have for every $n\in \mathbb {Z}$ , $f^n(z)=\pi \circ \sigma ^n(\underline {x})=\pi \circ \sigma ^n(\underline {y})$ and so $f^n(z)\in Z(x_n)\cap Z(y_n)$ , proving that $R_n\sim R_n^\prime $ for all $n\in \mathbb {Z}$ .

Theorem 6.2. The following holds for all $\varepsilon>0$ small enough.

  1. (1) $\widehat {\pi } \circ \widehat {\sigma }=f \circ \widehat {\pi }$ on $\widehat {\Sigma }^{\#}$ .

  2. (2) $\widehat {\pi }: \widehat {\Sigma }^{\#} \rightarrow O$ is continuous.

  3. (3) $\widehat {\pi }|_{\widehat {\Sigma }^{\#}}: \widehat {\Sigma }^{\#}\rightarrow O^{\#}$ is a finite-to-one surjective map.

Proof. (1) For any $\underline {R}\in \widehat {\Sigma }^{\#}$ , because f is a homeomorphism, we have

$$ \begin{align*} \begin{aligned} \{\widehat{\pi} \circ \widehat{\sigma}(\underline{R})\}&=\bigg\{\bigcap_{n=0}^{\infty}\overline{f^n(R_{-n+1})\cap\cdots\cap f^{-n}(R_{n+1})}\bigg\}=\bigg\{\bigcap_{n=0}^{\infty}\overline{\bigcap_{i=-n}^{n}f^{-i}(R_{i+1})}\bigg\}\notag\\ &\supset\bigg\{\bigcap_{n=0}^{\infty}\overline{\bigcap_{i=-n-2}^{n}f^{-(i+1)+1}(R_{i+1})}\bigg\}=\bigg\{f\bigg(\bigcap_{n=0}^{\infty}\overline{\bigcap_{i=-n-2}^{n}f^{-(i+1)}(R_{i+1})}\bigg)\bigg\}\notag\\ &=\bigg\{f\bigg(\bigcap_{n=0}^{\infty}\overline{\bigcap_{j=-n-1}^{n+1}f^{-j}(R_j)}\bigg)\bigg\}=\{f\circ\widehat{\pi}(\underline{R})\}. \end{aligned} \end{align*} $$

(2) If otherwise, then there is a $\xi>0$ so that for every $N>0$ , one can find $\underline {R}^{(N)}, \underline {S}^{(N)}\in \widehat {\Sigma }^{\#}$ with $R^{(N)}_i=S^{(N)}_i$ for all $i=-N,\ldots , N$ , but $d(\widehat {\pi }(\underline {R}^{(N)}),\widehat {\pi }(\underline {S}^{(N)}))\geq \xi $ . However, notice that $\widehat {\pi }(\underline {R}^{(N)}), \widehat {\pi }(\underline {S}^{(N)})\in \overline {\bigcap _{i=-N}^{N}f^{-i}(R^{(N)}_i)}$ , and hence by Lemma 6.5, there exists an $\varepsilon $ -rppo $\underline {x}=\{x^{(N)}_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ such that

$$ \begin{align*} \begin{aligned} &d(\widehat{\pi}(\underline{R}^{(N)}),\widehat{\pi}(\underline{S}^{(N)}))\\&\quad\leq \mathrm{diam}\bigg(\overline{\bigcap_{i=-N}^{N}f^{-i}(R^{(N)}_i)}\bigg)\notag\\ &\quad=\mathrm{diam}(\bigcap_{i=-N}^{N}f^{-i}(R^{(N)}_i))\notag\\ &\quad\leq8Q(x^{(N)}_N)\prod_{j=1}^{N}\|Df^{-1}|_{E^u(x^{(N)}_{j})}\|^{1/2}+8Q(x^{(N)}_{-N})\prod_{j=1}^{N}\|Df|_{E^s(x^{(N)}_{-j})}\|^{1/2}\underset{N \rightarrow \infty}{\longrightarrow}0. \end{aligned} \end{align*} $$

This leads to a contradiction.

(3) We first prove that $O^{\#}= \widehat {\pi }({\widehat {\Sigma }^{\#}})$ . The proof of $O^{\#}\subset \widehat {\pi }({\widehat {\Sigma }^{\#}})$ is the same as [Reference Sarig22, Theorem 12.5(3)]. So it suffices to establish the opposite direction $O^{\#}\supset \widehat {\pi }({\widehat {\Sigma }^{\#}})$ .

Suppose $\underline {R}=\{R_n\}_{n\in \mathbb {Z}}\in {\widehat {\Sigma }}^{\#}$ , proceeding as in the proof of Lemma 6.6, we can construct an $\varepsilon $ -rppo $\underline {x}\in \Sigma ^{\#}$ for $\underline {R}\in {\widehat {\Sigma }}^{\#}$ such that

$$ \begin{align*} z:=\widehat{\pi}(\underline{R})\in\bigcap_{n \geq 0} \overline{\bigcap_{i=-n}^{n}f^{-i}(Z(x_i))}, \end{align*} $$

that is, $f^n(z)\in \overline {Z(x_n)}$ for all $n\in \mathbb {Z}$ . Therefore, $d(f^n(z),x_n)\leq \mathrm {diam}(\overline {Z(x_n)})=\mathrm {diam}(Z(x_n)) \leq \tfrac 12Q(x_n)\leq \tfrac 12d(x_n,\partial O)$ , and we have

$$ \begin{align*} d(f^n(z),\partial O)\geq d(x_n,\partial O)-d(f^n(z),x_n)\geq \tfrac{1}{2}d(x_n,\partial O). \end{align*} $$

Thus, $z\in O^{\#}$ , that is, $\widehat {\pi }({\widehat {\Sigma }^{\#}})\subset O^{\#}$ .

Finally, we prove $\widehat {\pi }|_{\widehat {\Sigma }^{\#}}$ is finite-to-one. The proof is an adaptation of [Reference Lima and Sarig21, Theorem 5.6(5)] and [Reference Ben Ovadia6] to our context. The original proof [Reference Sarig22, Theorem 12.8] has a small error that was corrected in [Reference Lima and Sarig21].

Suppose $x\in O^{\#}$ , since $\widehat {\pi }({\widehat {\Sigma }^{\#}})=O^{\#}$ , x has a $\widehat {\pi }$ -preimage $\underline {R}\in {\widehat {\Sigma }^{\#}}$ such that $R_n=R$ for infinitely many positive n and $R_n=S$ for infinitely many negative n. Let $N:=N(R)N(S)$ and suppose by way of contradiction that there are $N+1$ different $\underline {R}^{(0)},\underline {R}^{(1)},\ldots , \underline {R}^{(N)}\in {\widehat {\Sigma }^{\#}}$ with $\underline {R}^{(0)}=\underline {R}$ and $\widehat {\pi }(\underline {R}^{(m)})=x$ for all $m=0,1,\ldots ,N$ . As produced in the proof of Lemma 6.6, we can construct for each $\underline {R}^{(m)}$ an $\varepsilon $ -rppo $\underline {x}^{(m)}\in \Sigma ^{\#}$ such that $\pi (\underline {x}^{(m)})=\widehat {\pi }(\underline {R}^{(m)})=x$ , and $R^{(m)}_n\subset Z(x^{(m)}_n)$ for all $n\in \mathbb {Z}$ and all $m=0,1,\ldots ,N$ .

Since the sequences $\{\underline {R}^{(m)}\}_{m=0}^N$ are distinct, there exists some $n_0>0$ such that

$$ \begin{align*} (R_{-n_0}^{(i)},\ldots, R_{n_0}^{(i)})\neq (R_{-n_0}^{(j)},\ldots, R_{n_0}^{(j)})\quad \text{for all } 0\leq i,j\leq N \text{ with } i\neq j. \end{align*} $$

Denote by $n^{+}$ the first $n\geq n_0$ such that $R_n=R$ , and by $n^{-}$ , the first $n\leq -n_0$ such that $R_n=S$ . Lemma 6.6 implies that there are at most $N=N(R)N(S)$ distinct choices of quadruple $(R_{n^{+}}^{(m)},x_{n^{+}}^{(m)};R_{n^{-}}^{(m)},x_{n^{-}}^{(m)} )$ for m. By the pigeonhole principle, there are $0\leq k,l\leq N$ with $k\neq l$ such that $(R,x_{n^+,R}):=(R_{n^{+}}^{(k)},x_{n^{+}}^{(k)})=(R_{n^{+}}^{(l)},x_{n^{+}}^{(l)})$ , $(S,x_{n^-,S}):=(R_{n^{-}}^{(k)},x_{n^{-}}^{(k)})=(R_{n^{-}}^{(l)},x_{n^{-}}^{(l)})$ , and

$$ \begin{align*} (R_{n^{-}}^{(k)},\ldots, R_{n^{+}}^{(k)})\neq (R_{n^{-}}^{(l)},\ldots,R_{n^{+}}^{(l)} ). \end{align*} $$

Now we apply the diamond argument [Reference Adler2, Lemma 6.7] to finish the proof of part (3). Fix $x\in \bigcap _{i=n^-}^{n^+}f^{-i}(R_i^{(k)})$ , $y\in \bigcap _{i=n^-}^{n^+}f^{-i}(R_i^{(l)})$ , and define $z_1,z_2$ by the equalities

$$ \begin{align*} f^{n^+}(z_1):=[f^{n^+}(x),f^{n^+}(y)]_{R}\quad \text{and}\quad f^{n^-}(z_2):=[f^{n^-}(x),f^{n^-}(y)]_{S}. \end{align*} $$

These points are uniquely defined by Proposition 6.6(2) since $f^{n^+}(x),f^{n^+}(y)\in R_{n^{+}}^{(k)}=R_{n^{+}}^{(l)}=R$ , $f^{n^-}(x),f^{n^-}(y)\in R_{n^{-}}^{(k)}=R_{n^{-}}^{(l)}=S$ . We will obtain a contradiction once we show that $z_1\neq z_2$ and $z_1= z_2$ .

First, note that $\{f^{n^+}(z_1)\}=W^u(f^{n^+}(x),R_{n^{+}}^{(k)})\cap W^s(f^{n^+}(y),R_{n^{+}}^{(l)})\subset W^u(f^{n^+}(x), R_{n^{+}}^{(k)})$ , by the Markov property (Proposition 6.6(3)), we have $z_1\in \bigcap _{i=n^-}^{n^+}f^{-i}(R_i^{(k)})$ . Similarly, since $\{f^{n^-}(z_2)\}=W^u(f^{n^-}(x),R_{n^{-}}^{(k)})\cap W^s(f^{n^-}(y),R_{n^{-}}^{(l)})\subset W^s(f^{n^-}(y),R_{n^{-}}^{(l)})$ , we have $z_2\in \bigcap _{i=n^-}^{n^+}f^{-i}(R_i^{(l)})$ . Therefore, we get $z_1\neq z_2$ for $(R_{n^{-}}^{(k)},\ldots , R_{n^{+}}^{(k)})\neq (R_{n^{-}}^{(l)},\ldots ,R_{n^{+}}^{(l)} )$ .

We now show that $z_1= z_2$ . Since $f^{n^+}(z_1)\in R\subset Z(x_{n^+,R})$ and $f^{n^-}(z_2)\in S\subset Z(x_{n^-,S})$ , there are $\underline {x}=\{x_n\}_{n\in \mathbb {Z}}, \underline {y}=\{y_n\}_{n\in \mathbb {Z}}\in \Sigma ^{\#}$ with $x_{n^+}=x_{n^+,R}, y_{n^-}=x_{n^-,S}$ such that $z_1=\pi (\underline {x})$ , $z_2=\pi (\underline {y})$ . Define $\underline {z}^\prime =\{z_n^\prime \}_{n\in \mathbb {Z}}\in \Sigma $ by

$$ \begin{align*} z^\prime_n=\begin{cases} y_n, & n \leq n^-, \\ x^{(k)}_n, & n^-\leq n\leq n^+,\\ x_n, & n\geq n^+.\\ \end{cases} \end{align*} $$

Since both $\underline {x}, \underline {y}\in \Sigma ^{\#}$ , also $\underline {z}^\prime \in \Sigma ^{\#}$ . We claim that $z_1=\pi (\underline {z}^\prime )=z_2$ .

In practice, note again that from $f^{n^+}(z_1)\in W^u(f^{n^+}(x),R_{n^{+}}^{(k)})$ and the Markov property (Proposition 6.6(3)), we have $f^{n^-}(z_1)\in W^u(f^{n^-}(x),R_{n^{-}}^{(k)})$ . Naturally, $f^{n^-}(z_2)\in W^u(f^{n^-}(x),R_{n^{-}}^{(k)})$ . Hence, we have by Definition 6.6,

$$ \begin{align*} f^{n^-}(z_1), f^{n^-}(z_2)\in W^u(f^{n^-}(x),R_{n^{-}}^{(k)})\subset W^u(f^{n^-}(x),Z(x_{n^{-}}^{(k)}))= W^u(f^{n^-}(x),Z(z^\prime_{n^{-}})). \end{align*} $$

By the symbolic Markov property (Proposition 6.4), for all $n\leq n^-$ , Proposition 5.2(2) and (4) imply that

$$ \begin{align*} f^{n}(z_1), f^{n}(z_2)\in W^u(f^{n}(x),Z(z^\prime_{n}))\subset \exp_{z^\prime_{n}}(S_{z^\prime_{n}})\quad\text{for all } n\leq n^-. \end{align*} $$

Similarly, we obtain that for all $n\geq n^+$ ,

$$ \begin{align*} f^{n}(z_1), f^{n}(z_2)\in W^s(f^{n}(x),Z(z^\prime_{n}))\subset \exp_{z^\prime_{n}}(S_{z^\prime_{n}})\quad\text{for all } n\geq n^+. \end{align*} $$

The next thing is to fix $n^-\leq n\leq n^+$ . Observe that we have $f^{n}(z_1), f^{n}(z_2)\in R_n^{(k)}\cup R_n^{(l)}\subset Z(x_n^{(k)})\cup Z(x_n^{(l)})$ . Since $\pi (\underline {x}^{(k)})=\pi (\underline {x}^{(l)})=x$ , we get $f^n(x)\in Z(x_n^{(k)})\cap Z(x_n^{(l)})$ . Then Lemma 6.3(1) implies that $Z(x_n^{(k)})\cup Z(x_n^{(l)})\subset \exp _{x_n^{(k)}}(S_{x_n^{(k)}})$ . Recalling $x_n^{(k)}=z^\prime _n$ for all $n^-\leq n\leq n^+$ , therefore,

$$ \begin{align*} f^{n}(z_1), f^{n}(z_2)\in \exp_{z^\prime_{n}}(S_{z^\prime_{n}}),\ n^-\leq n\leq n^+. \end{align*} $$

In conclusion, for this $\varepsilon $ -rppo $\underline {z}^\prime \in \Sigma ^{\#}$ , $f^{n}(z_1), f^{n}(z_2)\in \exp _{z^\prime _{n}}(S_{z^\prime _{n}})$ for all $n\in \mathbb {Z}$ . By the uniqueness of shadowing point, $z_1=z_2$ . This leads to a contradiction.

Acknowledgements

We are grateful to Professor Huyi Hu and the anonymous referees for useful comments and suggestions. The second author is the corresponding author. This work is supported by NSFC (Grant No. 11871120,12071082) and Natural Science Foundation of Chongqing (Grant No. cstc2021jcyj-msxmX0299).

References

Adler, R. L. and Weiss, B.. Similarity of Automorphisms of the Torus (Memoirs of the American Mathematical Society, 98). American Mathematical Society, Providence, RI, 1970.CrossRefGoogle Scholar
Adler, R. L.. Symbolic dynamics and Markov partitions. Bull. Amer. Math. Soc. (N.S.) 35(1) (1998), 156.CrossRefGoogle Scholar
Adler, R. L. and Weiss, B.. Entropy, a complete metric invariant for automorphisms of the torus. Proc. Natl. Acad. Sci. USA 57(6) (1967), 15731576.CrossRefGoogle ScholarPubMed
Araujo, E., Lima, Y. and Poletti, M.. Symbolic dynamics for nonuniformly hyperbolic maps with singularities in high dimension. Preprint, 2020, arXiv:2010.11808.Google Scholar
Barreira, L. and Pesin, Y. B.. Nonuniform Hyperbolicity: Dynamics of Systems with Nonzero Lyapunov Exponents (Encyclopedia of Mathematics and its Applications, 115). Cambridge University Press, Cambridge, 2007.CrossRefGoogle Scholar
Ben Ovadia, S.. Symbolic dynamics for non uniformly hyperbolic diffeomorphisms of compact smooth manifolds. J. Mod. Dyn. 13 (2018), 43113.CrossRefGoogle Scholar
Ben Ovadia, S.. Summable orbits. J. Mod. Dyn. 19 (2023), 625715.CrossRefGoogle Scholar
Bowen, R.. Equilibrium States and the Ergodic Theory of Anosov Diffeomorphisms (Lecture Notes in Mathematics, 470). Springer, Berlin, 1975, pp. 78104.CrossRefGoogle Scholar
Buzzi, J.. The degree of Bowen factors and injective codings of diffeomorphisms. J. Mod. Dyn. 16 (2020), 136.CrossRefGoogle Scholar
Chen, J., Hu, H. and Zhou, Y.. SRB measures for pointwise hyperbolic systems on open regions. Sci. China Math. 63(9) (2020), 16711720.CrossRefGoogle Scholar
Gurevich, B. M.. Topological entropy of a countable Markov chain. Dokl. Akad. Nauk 187(4) (1969), 715718.Google Scholar
Gurevich, B. M.. Shift entropy and Markov measures in the space of paths of a countable graph. Dokl. Akad. Nauk 192(5) (1970), 963965.Google Scholar
Hu, H.. Conditions for the existence of SBR measures for “almost Anosov” diffeomorphisms. Trans. Amer. Math. Soc. 352(5) (2000), 23312367.CrossRefGoogle Scholar
Hu, H. and Vaienti, S.. Absolutely continuous invariant measures for non-uniformly expanding maps. Ergod. Th. & Dynam. Sys. 29(4) (2009), 11851215.CrossRefGoogle Scholar
Hu, H. and Young, L.-S.. Nonexistence of SBR measures for some diffeomorphisms that are “almost Anosov”. Ergod. Th. & Dynam. Sys. 15(1) (1995), 6776.CrossRefGoogle Scholar
Kaloshin, V. Y.. Generic diffeomorphisms with superexponential growth of number of periodic orbits. Comm. Math. Phys. 211(1) (2000), 253271.CrossRefGoogle Scholar
Katok, A.. Bernoulli diffeomorphisms on surfaces. Ann. of Math. (2) 110(3) (1979), 529547.CrossRefGoogle Scholar
Lima, Y.. Symbolic dynamics for one dimensional maps with nonuniform expansion. Ann. Inst. H. Poincaré Anal. Non Linéaire 37(3) (2020), 727755.CrossRefGoogle Scholar
Lima, Y.. Symbolic dynamics for non-uniformly hyperbolic systems. Ergod. Th. & Dynam. Sys. 41(9) (2021), 25912658.CrossRefGoogle Scholar
Lima, Y. and Matheus, C.. Symbolic dynamics for non-uniformly hyperbolic surface maps with discontinuities. Ann. Sci. Éc. Norm. Supér. (4) 51(1) (2018), 138.CrossRefGoogle Scholar
Lima, Y. and Sarig, O. M.. Symbolic dynamics for three-dimensional flows with positive topological entropy. J. Eur. Math. Soc. (JEMS) 21(1) (2018), 199256.CrossRefGoogle Scholar
Sarig, O. M.. Symbolic dynamics for surface diffeomorphisms with positive entropy. J. Amer. Math. Soc. 26(2) (2013), 341426.CrossRefGoogle Scholar
Sinai, Y. G.. Construction of Markov partitions. Funct. Anal. Appl. 2(3) (1968), 245253.CrossRefGoogle Scholar
Sinai, Y. G.. Markov partitions and C-diffeomorphisms. Funct. Anal. Appl. 2(1) (1968), 6182.CrossRefGoogle Scholar