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Schramm-Loewner evolution contains a topological Sierpiński carpet when $κ$ is close to 8

Haoyu Liu, Zijie Zhuang

TL;DR

This work establishes that SLE$_\kappa$ curves with $\kappa$ near 8 almost surely have range structures containing a topological Sierpiński carpet, achieved by coupling SLE with the Gaussian free field via imaginary geometry and embedding Mandelbrot-type fractal percolation into the SLE trace. The main tool is a multi-scale fractal-percolation argument adapted to the dependent, IG-informed SLE setting, supported by precise regularity estimates as $\kappa\to 8$ and a coarse-grained analysis of the GFF. Consequently, the trace is almost surely conformally non-removable and the conformal welding problem for such SLEs has a non-unique solution; moreover, the adjacency graph of bubbles becomes disconnected in this regime. These results link fractal-percolation phenomena to the fine topological structure of SLE traces and have implications for the conformal welding and the broader understanding of SLE in the near-critical regime.

Abstract

We consider the Schramm-Loewner evolution (SLE$_κ$) for $κ\in (4,8)$, which is the regime where the curve is self-intersecting but not space-filling. We show that there exists $δ_0>0$ such that for $κ\in (8 - δ_0,8)$, the range of an SLE$_κ$ curve almost surely contains a topological Sierpiński carpet. Combined with a result of Ntalampekos (2021), this implies that in this parameter range, SLE$_κ$ is almost surely conformally non-removable, and the conformal welding problem for SLE$_κ$ does not have a unique solution. Our result also implies that for $κ\in (8 - δ_0,8)$, the adjacency graph of the complementary connected components of the SLE$_κ$ curve is disconnected.

Schramm-Loewner evolution contains a topological Sierpiński carpet when $κ$ is close to 8

TL;DR

This work establishes that SLE curves with near 8 almost surely have range structures containing a topological Sierpiński carpet, achieved by coupling SLE with the Gaussian free field via imaginary geometry and embedding Mandelbrot-type fractal percolation into the SLE trace. The main tool is a multi-scale fractal-percolation argument adapted to the dependent, IG-informed SLE setting, supported by precise regularity estimates as and a coarse-grained analysis of the GFF. Consequently, the trace is almost surely conformally non-removable and the conformal welding problem for such SLEs has a non-unique solution; moreover, the adjacency graph of bubbles becomes disconnected in this regime. These results link fractal-percolation phenomena to the fine topological structure of SLE traces and have implications for the conformal welding and the broader understanding of SLE in the near-critical regime.

Abstract

We consider the Schramm-Loewner evolution (SLE) for , which is the regime where the curve is self-intersecting but not space-filling. We show that there exists such that for , the range of an SLE curve almost surely contains a topological Sierpiński carpet. Combined with a result of Ntalampekos (2021), this implies that in this parameter range, SLE is almost surely conformally non-removable, and the conformal welding problem for SLE does not have a unique solution. Our result also implies that for , the adjacency graph of the complementary connected components of the SLE curve is disconnected.

Paper Structure

This paper contains 20 sections, 31 theorems, 77 equations, 10 figures.

Key Result

Theorem 1.1

All topological Sierpiński carpets are conformally non-removable.

Figures (10)

  • Figure 1: SLE$_\kappa$ curves arise as conformal welding interfaces Sheffield-zipperDMS21-LQG-MRT. Left: The case $\kappa \in (0,4]$. Right: The case $\kappa \in (4,8)$.
  • Figure 2: $N=4$ and on the event that $[0,1]^2$ is $\infty$-good. The regions in light-blue (resp. in light-blue or orange) are $[0,1]^2 \setminus A_1^\dagger$ (resp. $[0,1]^2 \setminus A_2^\dagger$). The set $A_2^*$ is obtained from $A_1^* \cap A_2^\dagger$ by further removing the green boxes.
  • Figure 3: The boundaries of two removed box clusters intersect at some point. Decreasing $p$ by any positive amount will almost surely merge these two clusters into one.
  • Figure 4: Left: The region in gray (resp. in gray or light-gray) represents the range of $\widetilde{\eta}$ stopped upon hitting $u$ (resp. $v$). In this figure, the point $u$ lies on the trace of $\eta$ whereas $v$ does not. Right: In Definition \ref{['def:n-good']}, the 0-good property requires that flow lines with different angles, after leaving the $\epsilon$-neighborhoods of starting points (marked in bold), are mutually non-intersecting. In this figure, the pair $(u_1,v_1)$ is admissible whereas $(u_2,v_2)$ is not.
  • Figure 5: Left: The exceptional point $v \in \eta^L(u)$ in Property \ref{['property:ig-dense']}. After hitting $v$ (and having filled the gray region), the curve $\widetilde{\eta}$ proceeds to fill $D_1$ (in light-blue) and then $D_2$ (in pink). Right: An illustration for the proof of Lemma \ref{['lem:flow-line-not-touch']}. If $\eta^L(w)$ and $\eta^R(w)$ intersect at $v \neq w$, then we can construct $w_1,w_2 \in B(x^{(n)},3\epsilon^n)$ that violates the $n$-good property of $x^{(n)}$.
  • ...and 5 more figures

Theorems & Definitions (66)

  • Theorem 1.1: Ntalampekos-carpet
  • Theorem 1.2
  • Theorem 1.3
  • Theorem 1.4
  • Remark 1.5
  • Theorem 1.6
  • Conjecture 1.7
  • Proposition 2.1
  • proof : Proof of Proposition \ref{['prop:carpet-fractal']}
  • Proposition 2.2
  • ...and 56 more