Bootstrap percolation on the random regular graph

被引:105
作者
Balogh, Jozsef
Pittel, Boris G.
机构
[1] Univ Illinois, Dept Math, Urbana, IL 61801 USA
[2] Ohio State Univ, Dept Math, Columbus, OH 43210 USA
关键词
cellular automata; percolation; random regular graph;
D O I
10.1002/rsa.20158
中图分类号
TP31 [计算机软件];
学科分类号
081202 ; 0835 ;
摘要
The k-parameter bootstrap percolation on a graph is a model of an interacting particle system, which can also be viewed as a variant of a cellular automaton growth process with threshold k >= 2. At the start, each of the graph vertices is active with probability p and inactive with probability I - p, independently of other vertices. Presence of active vertices triggers a bootstrap percolation process controlled by a recursive rule: an active vertex remains active forever, and a currently inactive vertex becomes active when at least k of its neighbors are active. The basic problem is to identify, for a given graph, p(-) and p(+) such that for p < p(-) (p > p(+) resp.) the probability that all vertices are eventually active is very close to 0 (1 resp.). The bootstrap percolation process is a deterministic process on the space of subsets of the vertex set, which is easy to describe but hard to analyze rigorously in general. We study the percolation on the random d-regular graph, d >= 3, via analysis of the process on the multigraph counterpart of the graph. Here, thanks to a "principle of deferred decisions," the percolation dynamics is described by a surprisingly simple Markov chain. Its generic state is formed by the counts of currently active and nonactive vertices having various degrees of activation capabilities. We replace the chain by a deterministic dynamical system, and use its integrals to show-via exponential supermartingales-that the percolation process undergoes relatively small fluctuations around the deterministic trajectory. This allows us to show existence of the phase transition within an interval [p(-)(n),p(+)(n)], such that (1)p(+/-)(n) -> p* = 1 - min(y epsilon(0,1)) y/P(Bin(d - 1, 1 -y) < k); (2)p(+)(n)-p(-)(n) is of order n(-1/2) for k < d(-1), and n(-epsilon n), (epsilon(n) down arrow 0, epsilon(n) log n -> infinity), for k = d - 1. Note that p* is the same as the critical probability of the process on the corresponding infinite regular tree. (c) 2006 Wiley Periodicals, Inc.
引用
收藏
页码:257 / 286
页数:30
相关论文
共 32 条
[1]   METASTABILITY EFFECTS IN BOOTSTRAP PERCOLATION [J].
AIZENMAN, M ;
LEBOWITZ, JL .
JOURNAL OF PHYSICS A-MATHEMATICAL AND GENERAL, 1988, 21 (19) :3801-3813
[2]  
Aldous DJ, 2000, RANDOM STRUCT ALGOR, V17, P79, DOI 10.1002/1098-2418(200009)17:2<79::AID-RSA1>3.0.CO
[3]  
2-W
[4]  
[Anonymous], P 22 IEEE ANN S FDN
[5]  
Aronson J, 1998, RANDOM STRUCT ALGOR, V12, P111, DOI 10.1002/(SICI)1098-2418(199803)12:2<111::AID-RSA1>3.0.CO
[6]  
2-#
[7]  
Balogh J, 1998, RANDOM STRUCT ALGOR, V13, P409, DOI 10.1002/(SICI)1098-2418(199810/12)13:3/4<409::AID-RSA11>3.0.CO
[8]  
2-U
[9]   Bootstrap percolation on the hypercube [J].
Balogh, J ;
Bollobás, B .
PROBABILITY THEORY AND RELATED FIELDS, 2006, 134 (04) :624-648
[10]   Sharp thresholds in Bootstrap percolation [J].
Balogh, J ;
Bollobás, B .
PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS, 2003, 326 (3-4) :305-312