In bootstrap percolation, a fraction p of the sites of a lattice is first randomly occupied, and then all occupied sites with fewer than a given integral number m of occupied neighbours are successively culled (rendered unoccupied) until either (a) a configuration of occupied sites, each with m or more occupied neighbours, ensues or (b) all sites of the lattice are vacated. The authors treat this problem as a function of m on square, triangular and cubic lattices by computer simulation. Various types of percolation transitions are discovered, including some which are discontinuous and some which are continuous but characterised by non-universal critical exponents.
Description
Bootstrap percolation transitions on real lattices
%0 Journal Article
%1 Kogut81
%A Kogut, P M
%A Leath, P L
%D 1981
%J Journal of Physics C: Solid State Physics
%K Bootstrap bootstrap lattices percolation real transitions
%N 22
%P 3187-3194
%R 10.1088/0022-3719/14/22/013
%T Bootstrap percolation transitions on real lattices
%U http://dx.doi.org/10.1088/0022-3719/14/22/013
%V 14
%X In bootstrap percolation, a fraction p of the sites of a lattice is first randomly occupied, and then all occupied sites with fewer than a given integral number m of occupied neighbours are successively culled (rendered unoccupied) until either (a) a configuration of occupied sites, each with m or more occupied neighbours, ensues or (b) all sites of the lattice are vacated. The authors treat this problem as a function of m on square, triangular and cubic lattices by computer simulation. Various types of percolation transitions are discovered, including some which are discontinuous and some which are continuous but characterised by non-universal critical exponents.
@article{Kogut81,
abstract = {In bootstrap percolation, a fraction p of the sites of a lattice is first randomly occupied, and then all occupied sites with fewer than a given integral number m of occupied neighbours are successively culled (rendered unoccupied) until either (a) a configuration of occupied sites, each with m or more occupied neighbours, ensues or (b) all sites of the lattice are vacated. The authors treat this problem as a function of m on square, triangular and cubic lattices by computer simulation. Various types of percolation transitions are discovered, including some which are discontinuous and some which are continuous but characterised by non-universal critical exponents.},
added-at = {2008-11-28T02:26:53.000+0100},
author = {Kogut, P M and Leath, P L},
biburl = {https://www.bibsonomy.org/bibtex/267a28321de291df921188810c53177e0/sidney},
description = {Bootstrap percolation transitions on real lattices},
doi = {10.1088/0022-3719/14/22/013},
interhash = {1cd0ca74d289b89a5f9fa195264c48d1},
intrahash = {67a28321de291df921188810c53177e0},
journal = {Journal of Physics C: Solid State Physics},
keywords = {Bootstrap bootstrap lattices percolation real transitions},
number = 22,
pages = {3187-3194},
timestamp = {2008-11-28T02:26:53.000+0100},
title = {Bootstrap percolation transitions on real lattices},
url = {http://dx.doi.org/10.1088/0022-3719/14/22/013},
volume = 14,
year = 1981
}