Multiple Random Walks and Interacting Particle Systems

  • Authors:
  • Colin Cooper;Alan Frieze;Tomasz Radzik

  • Affiliations:
  • Department of Computer Science, King's College London, London, UK WC2R 2LS;Department of Mathematical Sciences, Carnegie Mellon University, Pittsburgh, USA 15213;Department of Computer Science, King's College London, London, UK WC2R 2LS

  • Venue:
  • ICALP '09 Proceedings of the 36th Internatilonal Collogquium on Automata, Languages and Programming: Part II
  • Year:
  • 2009

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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.