Abstract
For a large class of transitive non-hyperbolic systems, we construct nonhyperbolic ergodic measures with entropy arbitrarily close to its maximal possible value. The systems we consider are partially hyperbolic with one-dimensional central direction for which there are positive entropy ergodic measures whose central Lyapunov exponent is negative, zero, or positive. We construct ergodic measures with zero central Lyapunov exponent whose entropy is positive and arbitrarily close to the topological entropy of the set of points with central Lyapunov exponent zero. This provides a restricted variational principle for nonhyperbolic (zero exponent) ergodic measures. The result is applied to the setting of \(\mathrm {SL}(2,\mathbb {R})\) matrix cocycles and provides a counterpart to Furstenberg’s classical result: for an open and dense subset of elliptic \(\mathrm {SL}(2,\mathbb {R})\) cocycles we construct ergodic measures with upper Lyapunov exponent zero and with metric entropy arbitrarily close to the topological entropy of the set of infinite matrix products with subexponential growth of the norm.
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Notes
Proximality holds if for every pair of points \(x,y\in \mathbb {S}^1\) there is \(\xi \in \Sigma _N\) so that \(|f_\xi ^n(x)-f_\xi ^n(y)|\rightarrow 0\) and \(|f_\xi ^{-n}(x)-f_\xi ^{-n}(y)|\rightarrow 0\) as \(n\rightarrow \infty \).
Furstenberg’s result states the dichotomy “positive Lyapunov exponent versus rigid dynamics”. As we are, by hypotheses, in a non-rigid context, this implies always positive exponent.
Our focus here is on as-large-as-possible entropy. The GIKN construction can be adapted and extended to produce nonhyperbolic measures with zero entropy and full support (see [7, 8, 10]). The method in [5] was modified in [9] to get nonhyperbolic measures with positive entropy and also full support. It was adapted also in [6] to deal with matrix cocycles. The constructions in this paper lay the foundations to construct nonhyperbolic measures with entropy as large as possible and also full support, following the ideas in [8, 9].
As in this paper we consider plenty of sequence spaces, we prefer this terminology.
It holds
$$\begin{aligned} \sup _{\mu :\mu \circ (\pi ^+\circ \pi _1)^{-1}=\nu ^+}h(F_\mathbf {A},\mu ) =h(\sigma ^+,\nu ^+)+\int _{\Sigma _N^+}h_\mathrm{top}(F_\mathbf {A},(\pi ^+\circ \pi _1)^{-1}(\xi ^+))\,d\nu ^+(\xi ^+). \end{aligned}$$It is straightforward to check that \(h_\mathrm{top}(F_\mathbf {A},(\pi ^+\circ \pi _1)^{-1}(\xi ^+))=0\) for every \(\xi ^+\).
The general definition of a coded system allows \(\mathcal {W}\) to be infinite. However, this will not be needed in this paper.
Note that this is slightly weaker than being uniquely decipherable as in [26, Definition 8.1.21].
We use the term simplified to avoid confusion with the term canonical defined above.
In [20], it is assumed that every measure in the sequence is uniformly distributed on a periodic orbit. The results in [32, Chapter 4] imply this criterion, and are in fact considerably more general, but this exact formulation does not appear there. For this reason we state this proposition and, for completeness, also its proof.
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Communicated by C. Liverani.
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This research has been supported [in part] by CAPES – Finance Code 001, by CNPq-grants, CNPq Projeto Universal, and E-16/2014 INCT/FAPERJ (Brazil) and by National Science Centre Grant 2019/33/B/ST1/00275 (Poland). The authors acknowledge the hospitality of IMPAN, IM-UFRJ, and PUC-Rio.
Appendix: Proof of Proposition 11.1
Appendix: Proof of Proposition 11.1
Given \(\phi :X\rightarrow \mathbb {R}\), denote
Given \(\varepsilon >0\), denote the upper topological limit of \((\Upsilon _{n,\phi ,\varepsilon })_n\) by \(\Upsilon _{\phi ,\varepsilon }\), that is,
We use the following fact that is straightforward to check.
Claim 11.2
For every continuous \(\phi :X\rightarrow \mathbb {R}\) and \(\varepsilon >0\) it holds
Lemma 11.3
For every continuous \(\phi :X\rightarrow \mathbb {R}\) and \(\varepsilon >0\) there exists a set \(\Xi _{\phi ,\varepsilon }\subset \Upsilon _{\phi ,\varepsilon }\) such that \(\varrho (\Xi _{\phi ,\varepsilon })>1-\varepsilon \) and
for every \(x\in \Xi _{\phi ,\varepsilon }\).
Proof
Given \(\phi \) and \(\varepsilon \), let \(L=L(\phi ,\varepsilon )\) and for \(\ell \ge L\) let \(N=N(\ell )\) be as in the hypothesis of the proposition. By Claim 11.2 and our hypothesis,
Every \(x\in \Upsilon _{\phi ,\varepsilon }\) is the limit of some sequence of points \(x_i\) in \(\Upsilon _{n_i,\phi ,\varepsilon }\), \(n_i\ge \ell \). Hence, for \(n_i\ge \ell \) sufficiently large, it holds
By our hypothesis on \(x_i\in \Upsilon _{n_i,\phi ,\varepsilon }\), it holds
Hence, for every \(x\in \Upsilon _{\phi ,\varepsilon }\) and \(\ell \ge 1\) sufficiently large it holds
Therefore, with the notation above, for every \(x\in \Upsilon _{\phi ,\varepsilon }\)
Applying the Birkhoff theorem to the invariant measure \(\varrho \), we get a set Z with \(\varrho (Z)=1\) so that at every \(z\in Z\) it holds \(\overline{\phi }(z)=\underline{\phi }(z)\). By the above, for every \(z\in \Xi _{\phi ,\varepsilon }\mathop {=}\limits ^{\mathrm{def}}Z\cap \Upsilon _{\phi ,\varepsilon }\) it holds \(|\overline{\phi }(z)-\phi (\varrho )|<3\varepsilon \) and \(\varrho (\Xi _{\phi ,\varepsilon })=\varrho (\Upsilon _{\phi ,\varepsilon })>1-\varepsilon \). This proves the lemma.
\(\square \)
Let us now prove that \(\varrho \) is ergodic. Take a dense set of continuous functions \(\{\phi _k\}_k\) and a summable sequence of positive numbers \((\varepsilon _k)_k\). As
by the Borel–Cantelli lemma, there is a set \(\Upsilon \) satisfying \(\varrho (\Upsilon )=1\) such that every \(x\in \Upsilon \) is contained in only finitely many sets \(\Upsilon _{\phi _k,\varepsilon _k}^c\). It follows that for every continuous \(\phi \) and \(x\in \Upsilon \) Birkhoff averages of \(\phi \) converge to \(\int \phi \,d\varrho \). This implies that \(\varrho \) is G-ergodic.
\(\square \)
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Díaz, L.J., Gelfert, K. & Rams, M. Variational Principle for Nonhyperbolic Ergodic Measures: Skew Products and Elliptic Cocycles. Commun. Math. Phys. 394, 73–141 (2022). https://doi.org/10.1007/s00220-022-04406-w
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DOI: https://doi.org/10.1007/s00220-022-04406-w