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A. Gandolfi, M. Keane, C. Newman (1992)
Uniqueness of the infinite component in a random graph with applications to percolation and spin glassesProbability Theory and Related Fields, 92
R. Durrett (1985)
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van Berg, Rachel Brouwer (2004)
Self-Organized Forest-Fires Near the Critical TimeCommunications in Mathematical Physics, 267
B. Bollobás, O. Riordan (2004)
The critical probability for random Voronoi percolation in the plane is 1/2Probability Theory and Related Fields, 136
J. Berg, R. Brouwer (2001)
Percolation, forest-fires and monomer-dimers
Van Berg, M. Keane (1984)
On the Continuity of the Percolation Probability Function
B. Bollobás, O. Riordan (2004)
Sharp thresholds and percolation in the planeRandom Structures & Algorithms, 29
Jacob Berg, Rachel Brouwer (2004)
Self‐destructive percolationRandom Structures & Algorithms, 24
R. Burton, M. Keane (1989)
Density and uniqueness in percolationCommunications in Mathematical Physics, 121
[A few years ago (see [1]) two of us introduced, motivated by the study of certain forest-fire processes, the self-destructive percolation model (abbreviated as sdp model). A typical configuration for the sdp model with parameters p and δ is generated in three steps: First we generate a typical configuration for the ordinary site percolation model with parameter p. Next, we make all sites in the infinite occupied cluster vacant. Finally, each site that was already vacant in the beginning or made vacant by the above action, becomes occupied with probability δ (independent of the other sites).]
Published: Jan 1, 2008
Keywords: Percolation; RSW results; box crossings; 60K35; 82B43
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