Title
Multiple Random Walks and Interacting Particle Systems
Abstract
We study properties of multiple random walks on a graph under various assumptions of interaction between the particles. To give precise results, we make our analysis for random regular graphs. The cover time of a random walk on a random r -regular graph was studied in [6], where it was shown with high probability (whp), that for r *** 3 the cover time is asymptotic to *** r n ln n , where *** r = (r *** 1)/(r *** 2). In this paper we prove the following (whp) results. For k independent walks on a random regular graph G , the cover time C G (k ) is asymptotic to C G /k , where C G is the cover time of a single walk. For most starting positions, the expected number of steps before any of the walks meet is $\theta_r n/\binom{k}{2}$. If the walks can communicate when meeting at a vertex, we show that, for most starting positions, the expected time for k walks to broadcast a single piece of information to each other is asymptotic to 2*** r n (ln k )/k , as k ,n *** ***. We also establish properties of walks where there are two types of particles, predator and prey, or where particles interact when they meet at a vertex by coalescing, or by annihilating each other. For example, the expected extinction time of k explosive particles (k even) tends to (2ln 2) *** r n as k *** ***. The case of n coalescing particles, where one particle is initially located at each vertex, corresponds to a voter model defined as follows: Initially each vertex has a distinct opinion, and at each step each vertex changes its opinion to that of a random neighbour. The expected time for a unique opinion to emerge is the expected time for all the particles to coalesce, which is asymptotic to 2 *** r n . Combining results from the predator-prey and multiple random walk models allows us to compare expected detection time in the following cops and robbers scenarios: both the predator and the prey move randomly, the prey moves randomly and the predators stay fixed, the predators move randomly and the prey stays fixed. In all cases, with k predators and *** prey the expected detection time is *** r H *** n /k , where H *** is the ***-th harmonic number.
Year
DOI
Venue
2009
10.1007/978-3-642-02930-1_33
ICALP (2)
Keywords
Field
DocType
interacting particle systems,c g,k predator,k explosive particle,random regular graph,cover time c g,expected time,ln k,detection time,cover time,k independent walk,multiple random walks,harmonic number,interacting particle system,random walk,regular graph
Discrete mathematics,Random regular graph,Particle system,Combinatorics,Vertex (geometry),Random walk,Harmonic number,Expected value,Regular graph,Voter model,Mathematics
Conference
Volume
ISSN
Citations 
5556
0302-9743
7
PageRank 
References 
Authors
0.68
11
3
Name
Order
Citations
PageRank
Colin Cooper185791.88
Alan M. Frieze24837787.00
Tomasz Radzik3109895.68