Stationary distribution for spinning reflecting diffusions

Abstract

Thesis (Ph.D.)--University of Washington, 2012This dissertation studies two different types of interaction of diffusion processes with the boundary of a domain DsubRRnDsubRR^n, which is assumed to be bounded, and of class C2(RRn)C^2(RR^n). The first process that is studied is obliquely reflected Brownian motion, and it is constructed as the unique Hunt process XX properly associated with the following Dirichlet form: \begin{align} \label{eq:abs_df} \tag{1} \E(u,v) = \frac12\int_D \nabla u\nabla(u\rho) dx + \frac12\int_D \nabla u \cdot\vec{\tau}\ v\ \rho(x)\sigma(dx), \end{align} where \vec\tau:\partial D\to\RR^n is tangential to βˆ‚D\partial D, and u,vu,v belong to the Sobolev space W1,2(D)W^{1,2}(D). The reference measure ρ(x)dx\rho(x)dx is assumed to be given by a harmonic function ρ\rho whose gradient βˆ‡Ο\nabla\rho is uniformly bounded. It is shown that such process XX admits a Skorohod decomposition \begin{align} \label{eq:abs_skorohod} \tag{2} dX_t = dB_t + [\vec{n}+\vec\tau](X_t)dL_t. \end{align} Moreover, we show that the unique stationary distribution of XX is the measure given by ρ(x)dx\rho(x)dx. In the second part of the dissertation, we present a new reflection process XtX_t in a bounded domain DD of class C^2(\RR^n) that behaves very much like oblique reflected Brownian motion, except that the directions of reflection depend on an external parameter StS_t called spin. The spin is allowed to change only when the process XtX_t is on the boundary of DD. The pair (X,S)(X,S) is called spinning Brownian motion and is found as the unique strong solution to the following stochastic differential equation: % %Let DβŠ†RnD\subseteq\mathbb{R}^n be an open C2C^2 domain, and let BtB_t be a nn-dimensional Brownian motion. A pair (Xt,St)(X_t,S_t) is called spinning Brownian motion (sBM) if it solves the following stochastic differential equation \begin{align} \label{eq:abs_sbm} \tag{3} \left\{ \begin{array}{rl} dX_t &= \sigma(X_t)dB_t + \vec{n}(X_t)dL_t + \vec \tau (X_t,S_t)dL_t \\ dS_t &= \spar{\vec{g}(X_t) - S_t } dL_t \end{array} \right. \end{align} where LtL_t is the local time process of XtX_t, nβƒ—\vec{n} is the interior unit normal to βˆ‚D\partial D, and Ο„βƒ—\vec\tau is a vector field perpendicular to n^\hat n. The function Οƒ(β‹…)\sigma(\cdot) is a non-degenerate (nΓ—n)(n\times n)-matrix valued function, and Ο„βƒ—(β‹…)\vec{\tau}(\cdot) and gβƒ—(β‹…)\vec g(\cdot) are Lipschitz bounded vector fields. % We prove that a unique strong solution to \eqref{eq:abs_sbm} exists as the limit of a family of processes (X^\e,S^\e) that satisfy an equation like \eqref{eq:abs_sbm}, but in which the spin component dSdS has a noise \e dW. With this added noise, the process (X^\e,S^\e) is an obliquely reflected Brownian motion in an unbounded domain. % It is also shown that spinning Brownian motion has a unique stationary distribution. The main tool of the proof is excursion theory, and an identification of the Local time of XtX_t as a component of an exist system for XtX_t

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Last time updated on 28/06/2013

This paper was published in DSpace at The University of Washington.

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