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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 $α(R) = 0$.

Multifractal spectrum of branching random walks on free groups

TL;DR

This work analyzes the multifractal structure of BRWs on free groups in the transient regime , identifying a detailed spectrum for the limit set on . 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 in the admissible range , , and there exists a unique with ; moreover, in the subcritical subcase () one has , while at the critical point () the phase transition yields . 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 is transient if and only if the mean offspring number does not exceed , the reciprocal of the spectral radius of the underlying random walk. In this regime, the limit set -- consisting of all ends of to which the BRW's particle trajectories converge -- is a proper random subset of the boundary . Hueter and Lalley (2000) determined the Hausdorff dimension of and proved that , with equality possible only when . In this paper, we further extend this study by conducting a multifractal analysis of the limit set . We obtain the Hausdorff dimensions of the subfractals , which consist of all ends of approached by particle trajectories escaping at rate . Notably, there exists a unique such that Moreover, an interesting phase transition occurs: for while .
Paper Structure (27 sections, 31 theorems, 315 equations, 1 figure)

This paper contains 27 sections, 31 theorems, 315 equations, 1 figure.

Key Result

Theorem 1.1

Let $r \in (1,R]$. Almost surely for any $\alpha \in [0,1]$, $\Lambda_r(\alpha)$ is nonempty if and only if $\alpha \in I(r)$. In this case, the Hausdorff dimension of $\Lambda_r(\alpha)$ is given by Here, $\alpha=0$ is permissible only when $r=R$, in which case the expression $\frac{\ln R - L^{*}(0)}{0}$ should be interpreted as $\lim_{\alpha \downarrow 0} \frac{L^{*}(0) - L^{*}(\alpha)}{\alpha}

Figures (1)

  • Figure 1: Illustration for $\alpha(r)$ in subcritical case $1 < r < R$ (left) and critical case $r = R$ (right).

Theorems & Definitions (59)

  • Theorem 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Lemma 2.1: LS97
  • Proposition 2.2: Lal91
  • Remark 2.3
  • Lemma 2.4
  • Proposition 2.5: L93
  • Lemma 2.6: HL00
  • Lemma 2.7
  • ...and 49 more