skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Probabilistic bootstrap percolation

Journal Article · · Journal of Statistical Physics; (United States)
DOI:https://doi.org/10.1007/BF01053606· OSTI ID:6652531
 [1]
  1. Univ. of Oxford (United Kingdom)

In bootstrap percolation, sites are occupied with probability p, but those with less than m occupied first neighbors are removed. This culling process is repeated until a stable configuration (all occupied sites have at least m occupied first neighbors or the who lattice is empty) is achieved. For m [ge] m, the transition is first order, while for m < m it is second order, with m-dependent exponents. In probabilistic bootstrap percolation sites have probability r or (1 - r) of being m- or m[prime]-sites, respectively m-sites are those which need at least Bethe lattices, where an exact solution is available. For m = 2 and m[prime] = 3, the transition changes from second to first order at r[sup 1] = 1/2, and the exponent [beta] is different for r < 1/2, r = 1/2, and r > 1/2. The same qualitative behavior is found for m = 1 and m[prime] = 3. On the other hand, for m = 1 and m[prime] = 2 the transition is always second order, with the same exponents of m = 1, for any value of r > 0. We found, for m = z - 1 and m[prime] = z, where z is the coordination number of the lattice, that p[sub c] = 1 for a value of r which depends on z, but is always above zero. Finally, we argue that, for bootstrap percolation on real lattices, the exponents v and [beta] for m = 2 and m = 1 are equal, for dimensions below 6.

OSTI ID:
6652531
Journal Information:
Journal of Statistical Physics; (United States), Vol. 70:3-4; ISSN 0022-4715
Country of Publication:
United States
Language:
English