Reflected Brownian motion In probability theory , reflected Brownian motion is a Wiener process in a space with reflecting boundaries. RBMs have been shown to describe queueing models experiencing heavy traffic as first proposed by Kingman and proven by Iglehart and Whitt .Definition A d –dimensional reflected Brownian motion Z is a stochastic process on uniquely defined by where X is an unconstrained Brownian motion and with Y a d –dimensional vector where Y is continuous and non–decreasing with Y = 0 Y j only increases at times for which Z j = 0 for j = 1,2,...,d Z ∈ , t ≥ 0. The reflection matrix describes boundary behaviour. In the interior of the process behaves like a Wiener process, on the boundary "roughly speaking, Z is pushed in direction R j whenever the boundary surface is hit, where R j is the j th column of the matrix R ."Stability conditions are known for RBMs in 1, 2, and 3 dimensions . "The problem of recurrence classification for SRBMs in four and higher dimensions remains open." In the special case where R is an M-matrix then necessary and sufficient conditions for stability are R is a non-singular matrix and R −1 μ < 0. One dimension The marginal distribution of a one-dimensional Brownian motion starting at 0 restricted to positive values with drift μ and variance σ 2 is for all t ≥ 0, which yields when taking t → ∞ an exponential distribution For fixed t , the distribution of Z coincides with the distribution of the running maximum M of the Brownian motion, But be aware that the distributions of the processes as a whole are very different. In particular, M is increasing in t , which is not the case for Z . The heat kernel for reflected Brownian motion at : For the plane aboveMultiple dimensions The stationary distribution of a reflected Brownian motion in multiple dimensions is tractable analytically when there is a product form stationary distribution , which occurs when the process is stable and where D = diag . In this case the probability density function is where η k = 2μ k γ k /Σ kk and γ = R −1 μ . Closed-form expressions for situations where the product form condition does not hold can be computed numerically as described below in the simulation section.Simulation One dimension In one dimension the simulated process is the absolute value of a Wiener process. The following MATLAB program creates a sample path. %rbm.m n=10^4; h=10^; t=h.*; mu=-1; X=zeros; M=X; B=X; B=3; X=3; for k=2:n+1 Y=sqrt*randn; U=rand; B=B+mu*h-Y; M=/2; X=max; end subplot plot; subplot plot; The error involved in discrete simulations has been quantified.Multiple dimensions allows simulation of steady state RBMs.Feller described possible boundary condition for the process
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