2021
DOI: 10.1007/s10955-020-02697-8
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Fixation for Two-Dimensional $${\mathcal {U}}$$-Ising and $${\mathcal {U}}$$-Voter Dynamics

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Cited by 4 publications
(6 citation statements)
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“…If r > d, on the other hand, then it is not hard to see that p c (Z d n , N d r ) → 1 as n → ∞, since an uninfected copy of {0, 1} d cannot be infected in the process. Similar results have been proved for some other families of automata in two dimensions [16,31,32,34], and weaker bounds are known for a small number of specific three-dimensional update families [13,35].…”
Section: Introductionsupporting
confidence: 77%
“…If r > d, on the other hand, then it is not hard to see that p c (Z d n , N d r ) → 1 as n → ∞, since an uninfected copy of {0, 1} d cannot be infected in the process. Similar results have been proved for some other families of automata in two dimensions [16,31,32,34], and weaker bounds are known for a small number of specific three-dimensional update families [13,35].…”
Section: Introductionsupporting
confidence: 77%
“…In particular, the the upper bound for the second case in (6) follows. Therefore, it only remains to cover the first case c = a + b when r − c ∈ {3, .…”
Section: Proof Of Theorem 11: Upper Boundsmentioning
confidence: 97%
“…The study of bootstrap processes on graphs was initiated in 1979 by Chalupa, Leath and Reich [11], and is motivated by problems arising from statistical physics, such as the Glauber dynamics of the zero-temperature Ising model, and kinetically constrained spin models of the liquid-glass transition (see, e.g., [6,16,[18][19][20]). The r-neighbour bootstrap process on a locally finite graph G is a monotone cellular automata on the configuration space {0, 1} V (G) , (we call vertices in state 1 "infected"), evolving in discrete time in the following way: 0 becomes 1 when it has at least r neighbours in state 1, and infected vertices remain infected forever.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper we generalize (5) by showing that the critical length is doubly exponential in p for each r ∈ {c+b+1, . .…”
Section: Introductionmentioning
confidence: 96%
“…The study of bootstrap processes on graphs was initiated in 1979 by Chalupa, Leath and Reich [10], and is motivated by problems arising from statistical physics, such as the Glauber dynamics of the zero-temperature Ising model, and kinetically constrained spin models of the liquid-glass transition (see, e.g., [5,15,[18][19][20]). The r-neighbour bootstrap process on a locally finite graph G is a monotone cellular automata on the configuration space {0, 1} V (G) , (we call vertices in state 1 "infected"), evolving in discrete time in the following way: 0 becomes 1 when it has at least r neighbours in state 1, and infected vertices remain infected forever.…”
Section: Introductionmentioning
confidence: 99%