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UW Math Probability Seminar, 2001-2002![]()
SPRING SEMESTER 2002
Thursdays in 901 Van Vleck Hall at 2:25 pm unless otherwise noted
References: Adler, R.J. (1981) The geometry of random fields, Wiley, New York. Chung, M.K., Worsley, K.J., Paus, T., Robbins, S., Taylor, J., Giedd, J.N., Rapoport, J.L., Evans, A.C. (2002) Tensor-based surface morphometry, Department TR 1049 (http://www.stat.wisc.edu/~mchung). Worsley, K.J., Evans, A.C., Marrett, S., Neelin, P. (1992) A Three-Dimensional Statistial Analysis for CBF Activation Studies in Human Brain. Human Brain Mapping, 4:58-73. Worsley, K.J., Marrett, S., Neelin, P., Vandal, A.C., Friston, K.J., Evans, A.C. (1996) A unified statistial approach for determining significant signals in iames of cerebral activation. Human Brain Maping, 4:58-73.
There will be a brief orgnizational meeting after the seminar. The Asymmetric One-Dimensional Constrained Ising Model: Rigorous Results Our proof combines several ingredients: (i) The Poincare comparison method, whose use involves analyzing the combinatorial structure of transition paths. (ii) Invention of a "long-range wave" process for comparison purposes, and its analysis via coupling and exponential martingales. (iii) For the lower bound, invention of an approximate "dual" process of coalescing random jumps and its analysis.
Zero-Temperature Dynamics and Critical Percolation Scaling Limits I will give a brief survey of some results, conjectures and open problems concerning zero-temperature stochastic Ising models, and then focus on the analysis of the continuum scaling limit of some two-dimensional dependent percolation models generated by such interacting particle systems. The scaling limit of those percolation models is shown to be the same as that of critical (independent) site percolation on the triangular lattice, whose existence and conformal invariance properties have been recently proved by S. Smirnov.
Second-class Particles in Asymmetric Exclusion Processes We describe what second-class particles are in exclusion processes, and discuss two interesting things about them: (1) Paths of second-class particles converge to characteristics and shocks of the macroscopic p.d.e. of the system, and (2) Second-class particles can be used to prove central limit theorems for the process.
Stochastic Equations for Spatial Birth and Death Processes, part I
The Weak/Strong Survival Transition in the Contact Process on a Tree The contact process on a homogeneous tree of degree three or greater is known to have three distinct phases: an extinction phase, a weak survival phase, and a strong survival phase. The existence of two qualitatively different survival phases is the most striking feature of the process, as the contact process on the integer lattice, in any dimension, exhibits only one survival phase (strong survival). Thus, the contact process on a homogeneous tree exhibits a phase transition, from weak to strong survival, of a different character than the phase transition for the contact process on the integer lattices. I shall discuss certain features of this phase transition, and compare it with similar phase transitions in other stochastic processes.
Reflected Backward Stochastic Differential Equations, Variational Inequalities and Dirichlet Problems
Large Deviations of Price Equilibria of Random Economic Systems
Refinement of a General Non-convex Large Deviations Result and Applications We relax certain assumptions in our recent large deviation result for a sequence of random elements in a vector space satisfying an "abstract exponential martingale condition." We give applications to large deviations of sequences of D[0,1] - valued random elements defined by certain recursive schemes.
Stochastic Equations for Spatial Birth and Death Processes, part II
Random Matrices and Determinantal Random Point Fields The purpose of the talk is to give an introduction to determinantal random point fields. Determinantal random point fields appear naturally in random matrix theory, probability theory, quantum mechanics, combinatorics, representation theory, and some other areas of mathematics and physics. The first part of the talk will be devoted to examples. In the second part we will concentrate on CLT type results for linear statistics. In particular, we will talk about the Costin-Lebowitz theorem for the counting function of particles.
Homogenization of stochastic Hamilton-Jacobi equations I shall briefly recall the classical results of P. L. Lions, G. Papanicolaou, S. R. S. Varadhan on homogenization of Hamilton-Jacobi equations with periodic Hamiltonian and also the results of F. Rezakhanlou and J. E. Tarver on the homogenization of stochastic Hamilton-Jacobi equations. Next I plan to consider the viscous version of the stochastic Hamilton-Jacobi equation and explain the connection between a special case of such a homogenization problem and large deviations for the quenched Brownian motion among Poissonian obstacles (A. Sznitman).
Brownian Traffic Modeling The use of Brownian approximations in the analysis of queueing systems has become a standard tool for queueing theorists. Such Brownian models offer good numerical approximations to conventional queueing systems ( fed by renewal-type traffic ) when the system is heavily utilized. In addition, even when the Brownian limit is analytically intractable, the temporal and spatial scalings associated with the corresponding limit theory offer tremendous insight into the behavior of the underlying queueing network. The existing literature has primarily focused on modeling contexts in which the inputs are renewal-like, by which we mean that the input processes have the time-homogeneity, short-range dependence, and light tails necessary to place the input stream in the " domain of attraction " of Brownian motion. In this talk, we will discuss several modeling environments in which more complex approximating processes are appropriate, and we shall describe some of the associated performance implications. In particular, we shall discuss Brownian traffic models for non-stationary queues ( incorporating " time-of-day " effects ), scheduled arrival processes, and perturbed renewal processes.
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