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Measure of maximal entropy for minimal Anosov actions

Tristan Humbert

TL;DR

The paper addresses identifying and characterizing the measure of maximal entropy for higher-rank Anosov actions by linking Carrasco–Rodriguez-Hertz’s geometric construction to the Ruelle–Taylor resonances framework of Guedes Bonthonneau–Weich et al. It shows that the topological entropy appears as the first resonance on the bundle of $d_s$-forms, with leaf measures providing resonant and co-resonant states, and proves a Bowen-type formula that expresses the MME in terms of sums over periodic torii. A uniform construction of the MME across the Weyl chamber is established, and a corollary counting periodic torii is derived, via a joint-propagator analysis and trace formula. These results generalize rank-one resonance methods to higher rank, linking spectral data and periodic orbit counting to equilibrium states for Anosov actions. The work advances the understanding of entropy, resonances, and periodic-orbit statistics in the setting of higher-rank hyperbolic dynamics with potential applications to non-locally symmetric examples.

Abstract

For a minimal Anosov $\mathbb R^κ$-action on a closed manifold, we study the measure of maximal entropy constructed by Carrasco and Rodriguez-Hertz in \cite{CarHer} and show that it fits into the theory of Ruelle-Taylor resonances introduced by Guedes Bonthonneau, Guillarmou, Hilgert, and Weich in \cite{GBGHW}. More precisely, we show that the topological entropy corresponds to the first Ruelle-Taylor resonance for the action on a certain bundle of forms and that the measure of maximal entropy can be retrieved as the distributional product of the corresponding resonant and co-resonant states. As a consequence, we prove a Bowen-type formula for the measure of maximal entropy and a counting result on the number of periodic torii.

Measure of maximal entropy for minimal Anosov actions

TL;DR

The paper addresses identifying and characterizing the measure of maximal entropy for higher-rank Anosov actions by linking Carrasco–Rodriguez-Hertz’s geometric construction to the Ruelle–Taylor resonances framework of Guedes Bonthonneau–Weich et al. It shows that the topological entropy appears as the first resonance on the bundle of -forms, with leaf measures providing resonant and co-resonant states, and proves a Bowen-type formula that expresses the MME in terms of sums over periodic torii. A uniform construction of the MME across the Weyl chamber is established, and a corollary counting periodic torii is derived, via a joint-propagator analysis and trace formula. These results generalize rank-one resonance methods to higher rank, linking spectral data and periodic orbit counting to equilibrium states for Anosov actions. The work advances the understanding of entropy, resonances, and periodic-orbit statistics in the setting of higher-rank hyperbolic dynamics with potential applications to non-locally symmetric examples.

Abstract

For a minimal Anosov -action on a closed manifold, we study the measure of maximal entropy constructed by Carrasco and Rodriguez-Hertz in \cite{CarHer} and show that it fits into the theory of Ruelle-Taylor resonances introduced by Guedes Bonthonneau, Guillarmou, Hilgert, and Weich in \cite{GBGHW}. More precisely, we show that the topological entropy corresponds to the first Ruelle-Taylor resonance for the action on a certain bundle of forms and that the measure of maximal entropy can be retrieved as the distributional product of the corresponding resonant and co-resonant states. As a consequence, we prove a Bowen-type formula for the measure of maximal entropy and a counting result on the number of periodic torii.

Paper Structure

This paper contains 12 sections, 19 theorems, 135 equations.

Key Result

Theorem 1

There exist families of leaf measures $\{m^u_{x}\mid x\in \mathcal{M}\}$ and $\{m^{cs}_{x}\mid x\in \mathcal{M}\}$ such that The product $m=cm^u\wedge m^{cs}$$($for some normalizing constant $c>0)$ defines a probability measure which is the measure of maximal entropy associated to any $A\in \mathcal{W}$. It is invariant for any $\varphi_1^A$ for $A\in \mathbf{a}$. Moreovoer, it is ergodic and has

Theorems & Definitions (36)

  • Definition 1.1
  • Definition 1.2
  • Theorem 1: Common measure of maximal entropy
  • Theorem 2: First resonance
  • Theorem 3: Bowen-type formula
  • Corollary 3.1: Torii counting
  • Proposition 2.1
  • proof
  • Lemma 2.2
  • Lemma 2.3
  • ...and 26 more