2016
DOI: 10.1007/s00440-015-0689-6
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The subleading order of two dimensional cover times

Abstract: Abstract. The ε-cover time of the two dimensional torus by Brownian motion is the time it takes for the process to come within distance ε > 0 from any point. Its leading order in the small ε-regime has been established by Dembo, Peres, Rosen and Zeitouni [Ann. of Math., 160 (2004)]. In this work, the second order correction is identified. The approach relies on a multi-scale refinement of the second moment method, and draws on ideas from the study of the extremes of branching Brownian motion.

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Cited by 61 publications
(91 citation statements)
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“…it was proved in the seminal paper [14] that α = 1 corresponds to the leading-order term of the expected cover time of the torus, see also [4] for the next leading term and [1] in the discrete case. In the following theorem, we prove that, given that the unit ball is unvisited by the Brownian motion, the law of the uncovered set around 0 at time t α is close to that of BRI(α):…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…it was proved in the seminal paper [14] that α = 1 corresponds to the leading-order term of the expected cover time of the torus, see also [4] for the next leading term and [1] in the discrete case. In the following theorem, we prove that, given that the unit ball is unvisited by the Brownian motion, the law of the uncovered set around 0 at time t α is close to that of BRI(α):…”
Section: Resultsmentioning
confidence: 99%
“…Proof. This is Proposition 8.10 of [4], with small adaptations, since we are working with torus of size n in the continuous setting as well. , we see that the trace of BRI(α) on B(r) can be obtained in the following way: take N ∼ Poisson(2α ln r) particles and place them on ∂B(r) uniformly and independently; then let these particles perform independent W -diffusions.…”
Section: Excursionsmentioning
confidence: 92%
“…We believe the route taken here also considerably streamlines the deep DPRZ-results on late and thin/thick points of BM [2], and, what is perhaps more, it will be useful in the study of the finer properties. In fact, our approach carries over, mutatis mutandis, to these issues as well: when backed with [1], the present notes suggest that in order to address lower order corrections, one "simply" needs to increase the number of scales.…”
mentioning
confidence: 87%
“…In particular, we implement the multiscale refinement of the second moment method emerged in the recent studies of Derrida's GREM and branching Brownian motion [5]. This tool brings to the fore the true process of covering [1] with the help of minimal infrastructure only; it also efficiently replaces the delicate tracking of points which DPRZ refer to as 'n-successful', and requires the use of finitely many scales only. All these features simplify substantially the proof of the DPRZ-theorem.…”
mentioning
confidence: 99%
“…This is a topic with rich ties to other objects such as the Gaussian free field [22]. There has been many works providing general bounds on the cover time, studying its evolution and its fluctuations in general [40,20,35,6,30], and in particular for the giant component of various random graphs [16], for trees [2,23], for the two dimensional torus [18,21,15,9] and for higher dimensional tori [8]. Feige [24,25] proved tight extremal upper and lower bounds on cover times of graphs (by SRW).…”
Section: Related Workmentioning
confidence: 99%