English

Randomized Geodesic Flow on Hyperbolic Groups

Probability 2026-02-03 v3 Dynamical Systems Group Theory Geometric Topology

Abstract

Motivated by Gromov's geodesic flow problem on hyperbolic groups GG, we develop in this paper an analog using random walks. This leads to a notion of a harmonic analog Θ\Theta of the Bowen-Margulis-Sullivan measure on 2G\partial^2 G. We provide three different but related constructions of Θ\Theta: 1) by moving the base-point along a quasigeodesic ray 2) by moving the base-point along random walk trajectories 3) directly as a push-forward under the boundary map to 2G\partial^2 G of a measure inherited from studying all bi-infinite random walk trajectories (with no restriction on base-point) on GZG^\mathbb{Z}. Of these, the third construction is the most involved and needs new techniques. It relies on developing a framework where we can treat bi-infinite random walk trajectories as analogs of bi-infinite geodesics on complete simply connected negatively curved manifolds. Geodesic flow on a hyperbolic group is typically not well-defined due to non-uniqueness of geodesics. We circumvent this problem in the random walk setup by considering \emph{all} trajectories. We thus get a well-defined discrete flow that we call the \emph{randomized geodesic flow}, given by the Z\mathbb{Z}-shift on bi-infinite random walk trajectories. The Z\mathbb{Z}-shift is the random analog of the time one map of the geodesic flow. As an analog of ergodicity of the geodesic flow on a closed negatively curved manifold, we establish ergodicity of the GG-action on (2G,Θ)(\partial^2G, \Theta). As a consequence of our construction, we prove that the randomized geodesic flow is exponentially mixing of all orders and establish a functional CLT.

Keywords

Cite

@article{arxiv.2411.14350,
  title  = {Randomized Geodesic Flow on Hyperbolic Groups},
  author = {Luzie Kupffer and Mahan Mj and Chiranjib Mukherjee},
  journal= {arXiv preprint arXiv:2411.14350},
  year   = {2026}
}

Comments

In V3, we added results on mixing and CLT, see Thm 2.6, Thm 2.7