2020
DOI: 10.1007/s00220-020-03705-4
|View full text |Cite
|
Sign up to set email alerts
|

Localization for Random Walks Among Random Obstacles in a Single Euclidean Ball

Abstract: Place an obstacle with probability 1−p independently at each vertex of Z d , and run a simple random walk until hitting one of the obstacles. For d ≥ 2 and p strictly above the critical threshold for site percolation, we condition on the environment where the origin is contained in an infinite connected component free of obstacles, and we show that for environments with probability tending to one as n → ∞ there exists a unique discrete Euclidean ball of volume d log 1/p n asymptotically such that the following… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
26
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
4
1

Relationship

2
3

Authors

Journals

citations
Cited by 10 publications
(26 citation statements)
references
References 57 publications
0
26
0
Order By: Relevance
“…Recently, it has been shown in [7,8] that conditioned on survival up to time n, the random walk stays in an island (determined by the environment) of diameter at most polylogarithmic in n during time [o(n), n]. Furthermore, at any deterministic time t ∈ [o(n), n], the random walk stays with high probability in a ball of radius asymptotically…”
Section: Model and Main Resultsmentioning
confidence: 99%
See 4 more Smart Citations
“…Recently, it has been shown in [7,8] that conditioned on survival up to time n, the random walk stays in an island (determined by the environment) of diameter at most polylogarithmic in n during time [o(n), n]. Furthermore, at any deterministic time t ∈ [o(n), n], the random walk stays with high probability in a ball of radius asymptotically…”
Section: Model and Main Resultsmentioning
confidence: 99%
“…Intuitively, the ball where the random walk will be localized should contain very few obstacles, or even no obstacle. It is proved in [8] that the volume proportion of obstacles inside the localizing ball is at most o(1), but it remains open to show that it actually contains no obstacle at all. Our first main result resolves this question.…”
Section: Model and Main Resultsmentioning
confidence: 99%
See 3 more Smart Citations