2012
DOI: 10.1214/10-aop620
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Biased random walks on Galton–Watson trees with leaves

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Cited by 46 publications
(139 citation statements)
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“…The common regeneration structure is based on the concept of super-regeneration times introduced in [2].…”
Section: A Common Regeneration Structurementioning
confidence: 99%
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“…The common regeneration structure is based on the concept of super-regeneration times introduced in [2].…”
Section: A Common Regeneration Structurementioning
confidence: 99%
“…On Galton-Watson trees with leaves (see [2,3,10,13]) or on supercritical percolation clusters (see [5,8,16]), the speed is certainly not increasing since it eventually vanishes. In these models, the slowdown of the walk can be explained by the presence of dead ends in the environment, which act as powerful traps.…”
Section: Introductionmentioning
confidence: 99%
“…Instead, the random environment arising in the percolation model creates traps which become stronger as the bias is increased, so that when the bias is set above a certain critical value, the speed of the biased random walk is zero [5,9,16]. This phenomenon, which has also been observed for the biased random walks on supercritical Galton-Watson trees [4,14] and a one-dimensional percolation model [1], is of physical significance, as it helps to explain how a particle could in some circumstances actually move more slowly when the strength of an external field, such as gravity, is greater [3].…”
Section: Introductionmentioning
confidence: 69%
“…Moreover, we can define an annealed law for X started from 0 by integrating out the environment, similarly to (4). To connect this model with the biased random walk on the random path introduced above, we suppose that the transition probabilities are defined by setting…”
Section: Biased Random Walk On a Self-avoiding Random Pathmentioning
confidence: 99%
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