Original article at: http://www.math.washington.edu/~ejpecp/viewarticle.php?id=2019

The time constant vanishes only on the percolation cone in directed first passage percolation

Yu Zhang, University of Colorado

Abstract

We consider the directed first passage percolation model on ${bf Z}^2$. In this model, we assign independently to each edge $e$ a passage time $t(e)$ with a common distribution $F$. We denote by $vec{T}({bf 0}, (r,theta))$ the passage time from the origin to $(r, theta)$ by a northeast path for $(r, theta)in {bf R}^+times [0,pi/2]$. It is known that $vec{T}({bf 0}, (r, theta))/r$ converges to a time constant $vec{mu}_F (theta)$. Let $vec{p}_c$ denote the critical probability for oriented percolation. In this paper, we show that the time constant has a phase transition at $vec{p}_c$, as follows: (1) If $F(0) < vec{p}_c$, then $vec{mu}_F(theta) >0$ for all $0leq thetaleq pi/2$. (2) If $F(0) = vec{p}_c$, then $vec{mu}_F(theta) >0$ if and only if $thetaneq pi/4$. (3) If $F(0)=p > vec{p}_c$, then there exists a percolation cone between $theta_p^-$ and $theta_p^+$ for $0leq theta^-_p< theta^+_p leq pi/2$ such that $vec{mu} (theta) >0$ if and only if $thetanotin [theta_p^-, theta^+_p]$. Furthermore, all the moments of $vec{T}({bf 0}, (r, theta))$ converge whenever $thetain [theta_p^-, theta^+_p]$. As applications, we describe the shape of the directed growth model on the distribution of $F$. We give a phase transition for the shape at $vec{p}_c$

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Original article at: http://www.math.washington.edu/~ejpecp/viewarticle.php?id=2019