Multifractal spectrum of branching random walks on free groups
Shuwen Lai, Heng Ma, Longmin Wang
TL;DR
This work analyzes the multifractal structure of BRWs on free groups in the transient regime $r\in(1,R]$, identifying a detailed spectrum for the limit set $\Lambda_r$ on $\partial\mathbb{F}$. By connecting the BRW trace to large-deviation principles for the word-length of the underlying random walk, the authors derive explicit formulas for the local fractal dimensions: for $\alpha>0$ in the admissible range $I(r)$, $\dim_{\mathrm{H}} \Lambda_r(\alpha)=\frac{\ln r - L^{*}(\alpha)}{\alpha}$, and there exists a unique $\alpha(r)$ with $\dim_{\mathrm{H}} \Lambda_r=\dim_{\mathrm{H}} \Lambda_r(\alpha(r))$; moreover, in the subcritical subcase ($r<R$) one has $\alpha(r)>0$, while at the critical point ($r=R$) the phase transition yields $\alpha(R)=0$. The proofs combine covering arguments with large-deviation estimates, a refined energy (Frostman) method to secure lower bounds on the level-set dimensions, and a zero-one law to ensure almost-sure determinism of the spectra. The results illuminate an energy–entropy trade-off governing the fractal geometry of BRW traces and establish a robust multifractal framework for BRWs on free groups, with implications for more general hyperbolic settings.
Abstract
A symmetric branching random walk (BRW) on a free group $\mathbb{F}$ is transient if and only if the mean offspring number $r$ does not exceed $R$, the reciprocal of the spectral radius of the underlying random walk. In this regime, the limit set $Λ_r$ -- consisting of all ends of $\mathbb{F}$ to which the BRW's particle trajectories converge -- is a proper random subset of the boundary $\partial \mathbb{F}$. Hueter and Lalley (2000) determined the Hausdorff dimension of $Λ_r$ and proved that $\dim_{\mathrm{H}} Λ_r \le (1/2)\dim_{\mathrm{H}} \partial \mathbb{F}$, with equality possible only when $r = R$. In this paper, we further extend this study by conducting a multifractal analysis of the limit set $Λ_r$. We obtain the Hausdorff dimensions of the subfractals $Λ_r(α) \subset Λ_r$, which consist of all ends of $\mathbb{F}$ approached by particle trajectories escaping at rate $α\in [0,1]$. Notably, there exists a unique $α(r) \in [0,1]$ such that \[ \dim_{\mathrm{H}} Λ_r = \dim_{\mathrm{H}} Λ_r(α(r)). \] Moreover, an interesting phase transition occurs: $α(r) > 0$ for $r < R$ while $α(R) = 0$.
