2008
DOI: 10.1103/physreve.78.051102
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Maximum distributions of bridges of noncolliding Brownian paths

Abstract: The one-dimensional Brownian motion starting from the origin at time t = 0, conditioned to return to the origin at time t = 1 and to stay positive during time interval 0 < t < 1, is called the Bessel bridge with duration 1. We consider the N -particle system of such Bessel bridges conditioned never to collide with each other in 0 < t < 1, which is the continuum limit of the vicious walk model in watermelon configuration with a wall. Distributions of maximum-values of paths attained in the time interval t ∈ (0,… Show more

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Cited by 38 publications
(54 citation statements)
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References 63 publications
(145 reference statements)
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“…Note that in [21] the authors derived these results by establishing connections with the theory of Young tableaux. Further studies have focused on the extreme properties of non-intersecting Brownian paths and bridges [26][27][28][29][30][31][32][33][34][35][36], relating them to the statistics of the largest eigenvalue of random matrices from Gaussian and Laguerre Orthogonal ensembles [34,35]. In this paper we consider N vicious walkers in the presence of the critical square root g(τ ) = W √ τ boundary.…”
Section: Introductionmentioning
confidence: 99%
“…Note that in [21] the authors derived these results by establishing connections with the theory of Young tableaux. Further studies have focused on the extreme properties of non-intersecting Brownian paths and bridges [26][27][28][29][30][31][32][33][34][35][36], relating them to the statistics of the largest eigenvalue of random matrices from Gaussian and Laguerre Orthogonal ensembles [34,35]. In this paper we consider N vicious walkers in the presence of the critical square root g(τ ) = W √ τ boundary.…”
Section: Introductionmentioning
confidence: 99%
“…The notion of "time" has evolved as well, so nowadays it can be a physical parameter, representing either the real time or, e.g., the length of a mesoscopic wire, the area of a string or an external temperature. The idea of a noisy walk of eigenvalues recently led also to such concepts as determinantal processes [2][3][4], Loewner diffusion [5], fluctuations of non-intersecting interfaces in thermal equilibrium [6] and the emergence of pre-shock spectral waves and universal scaling at the critical points of several random matrix models.…”
Section: Introductionmentioning
confidence: 99%
“…The Airy 2 process describes the evolution of the largest eigenvalue of H (centered and scaled). The Airy 2 process appears as a limit process in directed last passage percolation [7], non-intersecting Brownian bridges [4,[7][8][9][10][11][12][13], random tilings [14], interacting particle transport in 1D [15,16], quantum dynamics of fermions [17][18][19] and stochastic growth models, either discrete [4,20] or the continuum 1D Kardar-Parisi-Zhang (KPZ) equation [21,22] (for a review see [23][24][25]). In fact the Airy 2 process is a hallmark of the very broad 1D-KPZ universality class, which arises in all these models.…”
mentioning
confidence: 99%