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Annual Report 2008.pdf - SAMSI

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Knut Solna<br />

University of California-Irvine<br />

Department of Mathematics<br />

ksolna@math.uci.edu<br />

“Effective Transport Equations and Enhanced Backscattering in Random Waveguides” (with<br />

Josselin Garnier)<br />

Sheldon Wang<br />

New Jersey Institute of Technology<br />

Mathematical Sciences Department<br />

xwang@njit.edu<br />

“On Finite Element Modeling of Random Media”<br />

Yimin Xiao<br />

Michigan State University and <strong>SAMSI</strong><br />

Department of Statistics<br />

xiaoyimi@stt.msu.edu<br />

“Gaussian and Stable Random Fields: Dependence Structure and Fractal Properties”<br />

Isotropic and anisotropic random fields arise naturally in probability theory, statistics and have<br />

been applied in a wide range of scientific areas. Examples include fractional Brownian motion,<br />

solutions to stochastic heat and wave equations driven by Gaussian or stable noises, various<br />

spatiotemporal processes and many more. We provide general methods for studying the<br />

dependence structure, sample path regularity, and fractal properties of Gaussian and stable<br />

random fields.<br />

Ke Xu<br />

University of North Carolina-Chapel Hill<br />

Department of Mathematics<br />

xuke@email.unc.edu<br />

“On the Correspondence Between Creeping Flows of Viscous and Viscoelastic Fluids”<br />

From the wealth of exact solutions for Stokes flow of simple viscous fluids [Pozrikidis, Oxford<br />

University Press, Oxford, 1997, 222-311], the classical “viscous-viscoelastic correspondence”<br />

between creeping flows of viscous and linear viscoelastic materials yields exact viscoelastic<br />

creeping flow solutions. The correspondence is valid for an arbitrary prescribed source: of force,<br />

flow, displacement or stress; local or nonlocal; steady or oscillatory. Two special<br />

Stokes singularities, extended to viscoelasticity in this way, form the basis of<br />

modern microrheology [Mason and Weitz, Phys. Rev. Lett. 74 (1995), 1250-1253]: the Stokeslet<br />

(for a stationary point source of force) and the solution for a driven sphere. We amplify these

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