Eigenvalues of the laguerre process as non-colliding squared bessel processes

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作者
Konig, Wolfgang [1 ,2 ]
O'Connell, Neil [1 ]
机构
[1] Basic Res. Inst. in the Math. Sci., HP Laboratories Bristol
[2] Fachbereich Mathematik, MA 7-5, Technische Universität Berlin, Strasse des 17. Juni 136, D-10623 Berlin, Germany
来源
HP Laboratories Technical Report | 2001年 / BRIMS卷 / 07期
关键词
Brownian movement - Diffusion - Eigenvalues and eigenfunctions - Functions - Mathematical transformations - Matrix algebra;
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摘要
Let A (t) be a nxp matrix with independent standard complex Brownian entries and set M (t) = A (t)* A (t). This is a process version of the Laguerre ensemble and as such we shall refer to it as the Laguerre process. The purpose of this note is to remark that, assuming n > p- 1, the eigenvalues of M (t) evolve like p independent squared Bessel processes of dimension 2(n-p+ 1), conditioned (in the sense of Doob) never to collide. More precisely, the function h (χ ) = πi(χi - χj) is harmonic with respect to p independent squared Bessel processes of dimension 2(n-p+ 1), and the eigenvalue process has the same law as the corresponding Doob h-transform. In the case where the entries of A (t) are real Brownian motions, (M (t)) t ≥ 0 is the Wishart process considered by Bru [Br91]. There it is shown that the eigenvalues of M (t) evolve according to a certain diffusion process, the generator of which is given explicitly. An interpretation in terms of non-colliding processes does not seem to be possible in this case. We also identify a class of processes (including Brownian motion, squared Bessel processes and generalised Ornstein-Uhlenbeck processes) which are all amenable to the same h-transform, and compute the corresponding transition densities and upper tail asymptotics for the first collision time.
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