Table of Contents
Fetching ...

Sharp connectivity bounds for the vacant set of random interlacements

Subhajit Goswami, Pierre-François Rodriguez, Yuriy Shulzhenko

TL;DR

The paper analyzes the vacant set of random interlacements on $\mathbb{Z}^d$ ($d\ge 3$), deriving sharp lower bounds for the truncated two-point function $\tau_{u}^{\mathrm{tr}}(x)$ across all $u>0$, with sharpness up to the principal exponential order in $d=3$ and for $u\neq u_*$ in $d\ge 4$. The authors introduce a spatial tilting profile $f$ and construct a tilted interlacement measure $\widetilde{\mathbb{P}}_{f}$ to create oblique corridors that bias trajectories in a controlled, near-critical fashion, while maintaining a tractable entropy cost. A general lower-bound framework (LB-gen) for oblique connection–disconnection events is developed, and is combined with a robust coupling of tilted and untitled interlacements on local boxes (via soft local times and entrance-law comparisons) to transfer tilt-typical events to the original measure. The work yields a rotationally invariant, Euclidean-distance-based lower bound in $d=3$ and matching exponential-order lower bounds in higher dimensions, thereby completing sharp asymptotics in this percolation model and offering new tools for handling non-monotone, nonlocal percolation phenomena. The methods hinge on precise hitting-probability estimates for oblique sets and meticulous control of relative entropy, enabling a deep understanding of the scaling limit behavior near criticality.

Abstract

We consider percolation of the vacant set of random interlacements at intensity $u$ in dimensions three and higher, and derive lower bounds on the truncated two-point function for all values of $u>0$. These bounds are sharp up to principal exponential order for all $u$ in dimension three and all $u \neq u_\ast$ in higher dimensions, where $u_*$ refers to the critical parameter of the model, and they match the upper bounds derived in the article arXiv:2503.14497. In dimension three, our results further imply that the truncated two-point function grows at large distances $x$ at a rate that depends on $x$ only through its Euclidean norm, which offers a glimpse of the expected (Euclidean) invariance of the scaling limit at criticality. The rate function is atypical, it incurs a logarithmic correction and comes with an explicit pre-factor that converges to $0$ as the parameter $u$ approaches the critical point $u_*$ from either side. A particular challenge stems from the combined effects of lack of monotonicity due to the truncation in the super-critical phase, and the precise (rotationally invariant) controls we seek, that measure the effects of a certain "harmonic humpback" function. Among others, their derivation relies on rather fine estimates for hitting probabilities of the random walk in arbitrary direction $e$, which witness this invariance at the discrete level, and preclude straightforward applications of projection arguments.

Sharp connectivity bounds for the vacant set of random interlacements

TL;DR

The paper analyzes the vacant set of random interlacements on (), deriving sharp lower bounds for the truncated two-point function across all , with sharpness up to the principal exponential order in and for in . The authors introduce a spatial tilting profile and construct a tilted interlacement measure to create oblique corridors that bias trajectories in a controlled, near-critical fashion, while maintaining a tractable entropy cost. A general lower-bound framework (LB-gen) for oblique connection–disconnection events is developed, and is combined with a robust coupling of tilted and untitled interlacements on local boxes (via soft local times and entrance-law comparisons) to transfer tilt-typical events to the original measure. The work yields a rotationally invariant, Euclidean-distance-based lower bound in and matching exponential-order lower bounds in higher dimensions, thereby completing sharp asymptotics in this percolation model and offering new tools for handling non-monotone, nonlocal percolation phenomena. The methods hinge on precise hitting-probability estimates for oblique sets and meticulous control of relative entropy, enabling a deep understanding of the scaling limit behavior near criticality.

Abstract

We consider percolation of the vacant set of random interlacements at intensity in dimensions three and higher, and derive lower bounds on the truncated two-point function for all values of . These bounds are sharp up to principal exponential order for all in dimension three and all in higher dimensions, where refers to the critical parameter of the model, and they match the upper bounds derived in the article arXiv:2503.14497. In dimension three, our results further imply that the truncated two-point function grows at large distances at a rate that depends on only through its Euclidean norm, which offers a glimpse of the expected (Euclidean) invariance of the scaling limit at criticality. The rate function is atypical, it incurs a logarithmic correction and comes with an explicit pre-factor that converges to as the parameter approaches the critical point from either side. A particular challenge stems from the combined effects of lack of monotonicity due to the truncation in the super-critical phase, and the precise (rotationally invariant) controls we seek, that measure the effects of a certain "harmonic humpback" function. Among others, their derivation relies on rather fine estimates for hitting probabilities of the random walk in arbitrary direction , which witness this invariance at the discrete level, and preclude straightforward applications of projection arguments.

Paper Structure

This paper contains 7 sections, 16 theorems, 112 equations, 2 figures.

Key Result

Theorem 1.1

For all $u \in (0, \infty)$, When $d \ge 4$, for all $u \in (0,\infty)$, there exists $C = C(u, d) \in (0, \infty)$ such that for all $x \in \mathbb Z^d$,

Figures (2)

  • Figure 1: The "harmonic humpback" function $f$. The purple part is joint to both the red and blue curve, which distinguish sub- and super-critical regimes. In reality, each curve depicts a section orthogonal to the direction $e \in S^{d-1}$, which is arbitrary. The plateaux correspond to spatial regions at which trajectories arrive at roughly constant (but suitably modulated) intensity. For practical purposes the reader should think of $v \approx u$.
  • Figure 2: A configuration of cylinders in a generic direction $\bm{e = {x}/{|x|}}$. We illustrate a sample path contributing to the martingale $M_t$ introduced in \ref{['eq:hit-1']}. The point $z$ varies over all of $\widetilde{T}$, which includes the two 'stablilizing' rods (dashed). These are used to achieve the desired uniformity for the lower bound in \ref{['eq:mart-2']}. In reality, all lines and rectangles drawn are replaced by lattice approximations, cf. \ref{['eq:T_x']}-\ref{['eq:T_i']}.

Theorems & Definitions (32)

  • Theorem 1.1
  • Corollary 1.2
  • Proposition 2.1
  • proof
  • Lemma 2.2: $d = 3$
  • proof : Proof of Lemma \ref{['C:mart']}
  • Theorem 3.1
  • proof : Proof of Theorem \ref{['T:LB-RI']}
  • Remark 3.2: one-arm estimates
  • Proposition 4.1
  • ...and 22 more