Paths in Weyl chambers and random matrices

成果类型:
Article
署名作者:
Bougerol, P; Jeulin, T
署名单位:
Centre National de la Recherche Scientifique (CNRS); CNRS - National Institute for Mathematical Sciences (INSMI); Universite Paris Cite; Sorbonne Universite; Universite Paris Cite; Sorbonne Universite; Centre National de la Recherche Scientifique (CNRS); CNRS - National Institute for Mathematical Sciences (INSMI)
刊物名称:
PROBABILITY THEORY AND RELATED FIELDS
ISSN/ISSBN:
0178-8051
DOI:
10.1007/s004400200221
发表日期:
2002
页码:
517-543
关键词:
brownian-motion LIMIT-THEOREMS REPRESENTATION eigenvalues
摘要:
Baryshnikov [4] and Gravner, Tracy & Widom (15) have shown that the largest eigenvalue of a random matrix of the G.U.E. of order d has the same distribution as max(1greater than or equal tot1greater than or equal to...greater than or equal totd-1greater than or equal to0) [W-1(1) - W-1(t(1)) + W-2(t(1)) - W-2(t(2)) + ... + W-d(t(d-1))], where W = (W-1,...,W-d) is a d-dimensional Brownian motion. We provide a generalization of this formula to all the eigenvalues and give a geometric interpretation. For any Weyl chamber a(+) of an Euclidean finite-dimensional space a, we define a natural continuous path transformation T which associates to a path w in a a path Tw in (a) over bar (+). This transformation occurs in the description of the asymptotic behaviour of some deterministic dynamical systems on the symmetric space G/K where G is the complex group with chamber a(+). When a = R-d, a(+) = {(x(1),..., x(d)); x(1) > x(2) >...> x(d)} and if W is the Euclidean Brownian motion on a then TW is the process of the eigenvalues of the Dyson Brownian motion on the set of Hermitian matrices and (TW)(1) is distributed as the eigenvalues of the G.U.E.
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