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The largest slice of fractal percolation

Pablo Shmerkin, Ville Suomala

TL;DR

The paper determines exact thresholds for the appearance of $k$ collinear points in dyadic planar fractal percolation, showing a sharp transition at $p_k=2^{(-k-2)/k}$ for $k\ge3$ and that no $k$-point line exists at criticality. It combines discretization, first- and second-moment methods, and FKG-type arguments to prove nonexistence below the threshold and existence above it (conditioned on non-extinction), establishing a cascade of phase transitions as $k$ grows. In the critical case where the Hausdorff dimension is $1$, the largest linear slice is a Cantor-type set with zero Hausdorff dimension in the standard sense, but it attains positive size in refined gauge-based measures: for a suitable $\phi$, there exists a line with $\mathcal H^\phi(A\cap\ell)>0$, and $\mathcal H^\phi(A)<\infty$. The results extend to $m$-ary grids with $p_k=m^{(-k-2)/k}$ and the same dimension-threshold formula, highlighting a deep link between fractal percolation geometry and generalized Hausdorff measures.

Abstract

For each $k\ge 3$, we determine the dimensional threshold for planar fractal percolation to contain $k$ collinear points. In the critical case of dimension $1$, the largest linear slice of fractal percolation is a Cantor set of zero Hausdorff dimension. We investigate its size in terms of generalized Hausdorff measures.

The largest slice of fractal percolation

TL;DR

The paper determines exact thresholds for the appearance of collinear points in dyadic planar fractal percolation, showing a sharp transition at for and that no -point line exists at criticality. It combines discretization, first- and second-moment methods, and FKG-type arguments to prove nonexistence below the threshold and existence above it (conditioned on non-extinction), establishing a cascade of phase transitions as grows. In the critical case where the Hausdorff dimension is , the largest linear slice is a Cantor-type set with zero Hausdorff dimension in the standard sense, but it attains positive size in refined gauge-based measures: for a suitable , there exists a line with , and . The results extend to -ary grids with and the same dimension-threshold formula, highlighting a deep link between fractal percolation geometry and generalized Hausdorff measures.

Abstract

For each , we determine the dimensional threshold for planar fractal percolation to contain collinear points. In the critical case of dimension , the largest linear slice of fractal percolation is a Cantor set of zero Hausdorff dimension. We investigate its size in terms of generalized Hausdorff measures.
Paper Structure (12 sections, 11 theorems, 57 equations, 2 figures)

This paper contains 12 sections, 11 theorems, 57 equations, 2 figures.

Key Result

Theorem 1.1

Consider dyadic fractal percolation $A=A^{\text{perc}(p)}$ on $[0,1]^2$. Let $3\le k\in\mathbb{N}$.

Figures (2)

  • Figure 1: A realization of fractal percolation with $p=0.8$.
  • Figure 2: A possible selection of $R_i$ for $k=3$ and $m=2$. The unions of the squares of the same colour form two elements of $\mathcal{C}_2$.

Theorems & Definitions (21)

  • Theorem 1.1
  • Remark 1.2
  • Theorem 1.3
  • Remark 1.4
  • Lemma 2.1
  • Lemma 2.2
  • Lemma 2.3
  • proof
  • Proposition 3.1
  • proof : Proof of Theorem \ref{['thm:finite-intersections']} assuming Proposition \ref{['prop:discretized_statement']}
  • ...and 11 more