Abstract

We study the site version of (independent) first-passage percolation on the triangular lattice $\mathbb{T}$. Denote the passage time of the site $v$ in $\mathbb{T}$ by $t(v)$, and assume that $P(t(v)=0)=P(t(v)=1)=1/2$. Denote by $a_{0,n}$ the passage time from $\textbf{0}$ to $(n,0)$, and by $b_{0,n}$ the passage time from $\textbf{0}$ to the halfplane $\{(x,y):x\geq n\}$. We prove that there exists a constant $0<\mu<\infty$ such that as $n\rightarrow\infty$, $a_{0,n}/\log n\rightarrow \mu$ in probability and $b_{0,n}/\log n\rightarrow \mu/2$ almost surely. This result confirms a prediction of Kesten and Zhang (Probab. Theory Relat. Fields \textbf{107}: 137--160, 1997). The proof relies on the existence of the full scaling limit of critical site percolation on $\mathbb{T}$, established by Camia and Newman.

Highlights

  • Standard first-passage percolation (FPP) was introduced by Hammersley and Welsh [8] in 1965 as a model of fluid flow through a random medium

  • We study the site version of first-passage percolation on the triangular lattice T

  • Unless otherwise stated, we will focus on the site version of FPP on the triangular lattice T, which is defined precisely in the following, and the reason will be explained later

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Summary

Introduction

Standard first-passage percolation (FPP) was introduced by Hammersley and Welsh [8] in 1965 as a model of fluid flow through a random medium. When the annulus is very large, this quantity can be approximated well by the passage time defined analogously for the corresponding annulus with respect to Camia and Newman’s full scaling limit [3] (see Fig. 1). For this scaling limit, by the subadditive ergodic theorem we get a SLLN for the passage times of annuli, which can be used to approximate the passage times of the large and long annuli for the discrete model. Throughout this paper, C, C1, C2, . . . denote positive finite constants that may change from line to line or page to page according to the context

Preliminary results
Proof of theorem
Full Text
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