Abstract

The Dirichlet forms related to various infinite systems of interacting Brownian motions are studied. For a given random point field μ, there exist two natural infinite-volume Dirichlet forms (mathcal {E}^{mathsf {upr}},mathcal {D}^{mathsf {upr}}) and (mathcal {E}^{mathsf {lwr}},mathcal {D}^{mathsf {lwr}}) on L2(S,μ) describing interacting Brownian motions each with unlabeled equilibrium state μ. The former is a decreasing limit of a scheme of such finite-volume Dirichlet forms, and the latter is an increasing limit of another scheme of such finite-volume Dirichlet forms. Furthermore, the latter is an extension of the former. We present a sufficient condition such that these two Dirichlet forms are the same. In the first main theorem (Theorem 3.1) the Markovian semi-group given by (mathcal {E}^{mathsf {lwr}},mathcal {D}^{mathsf {lwr}}) is associated with a natural infinite-dimensional stochastic differential equation (ISDE). In the second main theorem (Theorem 3.2), we prove that these Dirichlet forms coincide with each other by using the uniqueness of weak solutions of ISDE. We apply Theorem 3.1 to stochastic dynamics arising from random matrix theory such as the sine, Bessel, and Ginibre interacting Brownian motions and interacting Brownian motions with Ruelle’s class interaction potentials, and Theorem 3.2 to the sine2 interacting Brownian motion and interacting Brownian motions with Ruelle’s class interaction potentials of {C_{0}^{3}} -class.

Highlights

  • An infinite system of interacting Brownian motions in Rd can be represented by an (Rd )Nvalued stochastic process X = (Xi)i∈N [10, 11, 14, 18]

  • Examples of universal stochastic dynamics are the sine, Bessel, and Ginibre interacting Brownian motions. They are limits of the stochastic dynamics related to N -particle systems with reversible random point fields that converge to those universal random point fields mentioned above

  • We present the infinite-dimensional stochastic differential equation (ISDE) describing the labeled dynamics given by Lemma 2.7

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Summary

Introduction

Lang constructed the infinite system of Brownian motions as a limit of stochastic dynamics in bounded domains SR by considering finite systems with another boundary condition [10, 11]. Assuming the uniqueness of weak solutions of Eq 1.4 under the foregoing well-behaved properties, we proved that these two limits of the weak solutions are the same This establishes the coincidence of the two Dirichlet forms (E lwr, D lwr) and (E upr, D upr) in the second main theorem (Theorem 3.2). Examples of universal stochastic dynamics are the sine, Bessel, and Ginibre interacting Brownian motions (see Section 7) They are limits of the stochastic dynamics related to N -particle systems with reversible random point fields that converge to those universal random point fields mentioned above.

Two Schemes of Dirichlet Forms
ISDE-Representation
Statements of the Main Results
Examples
Gibbs Measures with Ruelle-Class Potential
Ginibre Interacting Brownian Motion
Concluding Remarks and Questions
Full Text
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