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Noncolliding Brownian motions and Harish-Chandra formula
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Makoto Katori, Chuo university Hideki Tanemura, Chiba university |
Abstract
We consider a system of noncolliding Brownian motions
introduced in our previous paper,
in which the noncolliding condition is imposed
in a finite time interval $(0,T]$.
This is a temporally inhomogeneous diffusion process
whose transition probability density depends on a value of $T$,
and in the limit $T to infty$
it converges to a temporally homogeneous diffusion process
called Dyson's model of Brownian motions.
It is known that the distribution of particle positions in Dyson's model
coincides with that of eigenvalues of a Hermitian matrix-valued
process, whose entries are independent Brownian motions.
In the present paper we construct such a Hermitian matrix-valued process,
whose entries are sums of
Brownian motions and Brownian bridges given
independently of each other,
that its eigenvalues are identically distributed
with the particle positions of
our temporally inhomogeneous system of noncolliding Brownian motions.
As a corollary of this identification we derive the
Harish-Chandra formula for an integral over the unitary group.
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Full text: PDF
Pages: 112-121
Published on: September 23, 2003
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Electronic Communications in Probability. ISSN: 1083-589X |
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