2012
DOI: 10.1088/1751-8113/45/9/095003
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The height of watermelons with wall

Abstract: We derive asymptotics for the moments as well as the weak limit of the height distribution of watermelons with p branches with wall. This generalises a famous result of de Bruijn, Knuth and Rice [4] on the average height of planted plane trees, and results by Fulmek [13] and Katori et al. [19] on the expected value, respectively higher moments, of the height distribution of watermelons with two branches.The asymptotics for the moments depend on the analytic behaviour of certain multidimensional Dirichlet seri… Show more

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Cited by 15 publications
(7 citation statements)
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“…If one knows the limiting behaviour for one particular random walk then the same convergence is valid for all random walks satisfying the conditions in our theorems. For example, Feierl [12,13] has considered functionals max k≤n (x d + S d (k)) and max…”
Section: Corollary 3 For Every Fixedmentioning
confidence: 99%
“…If one knows the limiting behaviour for one particular random walk then the same convergence is valid for all random walks satisfying the conditions in our theorems. For example, Feierl [12,13] has considered functionals max k≤n (x d + S d (k)) and max…”
Section: Corollary 3 For Every Fixedmentioning
confidence: 99%
“…Let x N (t) denote the position of the rightmost Brownian motion in [0, 1], and define the random variable H N = max {x N (t), 0 < t < 1} specifying the maximum displacement. It was shown in [64,47,22] 25) whereF N (L) is specified by (2.17) with the particular proportionality constant…”
Section: Fluctuation Formulasmentioning
confidence: 99%
“…The noncolliding BM is equivalent to Dyson's BM model (with parameter β = 2) and the latter is known as an eigenvalue process of Hermitian matrix-valued BM [13,53,67,24,26,37,42,69,58,59]. Then the noncolliding RW has been attracted much attention as a discretization of models associated with the Gaussian random matrix ensembles [2,27,55,36,28,3,18,16]. Nagao and Forrester [55] studied a 'bridge' of noncolliding RW started from u 0 = (2j) N −1 j=0 at t = 0 and returned to the same configuration u 0 at time t = 2M, M ∈ N 0 .…”
Section: Constructionmentioning
confidence: 99%