TY - JOUR

T1 - Noncolliding Brownian motion and determinantal processes

AU - Katori, Makoto

AU - Tanemura, Hideki

N1 - Funding Information:
Acknowledgements The present authors would like to thank H. Osada, Y. Takahashi, A. Borodin and G. Olshanski for useful discussions on determinantal processes. M.K. is supported in part by the Grant-in-Aid for Scientific Research (KIBAN-C, No.17540363) of Japan Society for the Promotion of Science. H.T. is supported in part by the Grant-in-Aid for Scientific Research (KIBAN-C, No.19540114) of Japan Society for the Promotion of Science.

PY - 2007/10

Y1 - 2007/10

N2 - A system of one-dimensional Brownian motions (BMs) conditioned never to collide with each other is realized as (i) Dyson's BM model, which is a process of eigenvalues of hermitian matrix-valued diffusion process in the Gaussian unitary ensemble (GUE), and as (ii) the h-transform of absorbing BM in a Weyl chamber, where the harmonic function h is the product of differences of variables (the Vandermonde determinant). The Karlin-McGregor formula gives determinantal expression to the transition probability density of absorbing BM. We show from the Karlin-McGregor formula, if the initial state is in the eigenvalue distribution of GUE, the noncolliding BM is a determinantal process, in the sense that any multitime correlation function is given by a determinant specified by a matrix-kernel. By taking appropriate scaling limits, spatially homogeneous and inhomogeneous infinite determinantal processes are derived. We note that the determinantal processes related with noncolliding particle systems have a feature in common such that the matrix-kernels are expressed using spectral projections of appropriate effective Hamiltonians. On the common structure of matrix-kernels, continuity of processes in time is proved and general property of the determinantal processes is discussed.

AB - A system of one-dimensional Brownian motions (BMs) conditioned never to collide with each other is realized as (i) Dyson's BM model, which is a process of eigenvalues of hermitian matrix-valued diffusion process in the Gaussian unitary ensemble (GUE), and as (ii) the h-transform of absorbing BM in a Weyl chamber, where the harmonic function h is the product of differences of variables (the Vandermonde determinant). The Karlin-McGregor formula gives determinantal expression to the transition probability density of absorbing BM. We show from the Karlin-McGregor formula, if the initial state is in the eigenvalue distribution of GUE, the noncolliding BM is a determinantal process, in the sense that any multitime correlation function is given by a determinant specified by a matrix-kernel. By taking appropriate scaling limits, spatially homogeneous and inhomogeneous infinite determinantal processes are derived. We note that the determinantal processes related with noncolliding particle systems have a feature in common such that the matrix-kernels are expressed using spectral projections of appropriate effective Hamiltonians. On the common structure of matrix-kernels, continuity of processes in time is proved and general property of the determinantal processes is discussed.

KW - Determinantal processes

KW - Karlin-McGregor formula

KW - Matrix-kernels

KW - Multitime correlation functions

KW - Noncolliding Brownian motion

KW - Random matrix theory

KW - Spectral projections

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U2 - 10.1007/s10955-007-9421-y

DO - 10.1007/s10955-007-9421-y

M3 - Article

AN - SCOPUS:36448991470

SN - 0022-4715

VL - 129

SP - 1233

EP - 1277

JO - Journal of Statistical Physics

JF - Journal of Statistical Physics

IS - 5-6

ER -