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Dive into the research topics where Russell M. Brown is active.

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Featured researches published by Russell M. Brown.


Applicable Analysis | 2006

Identifiability at the boundary for first-order terms

Russell M. Brown; Mikko Salo

Let Ω be a domain in R n whose boundary is C 1 if n≥3 or C 1,β if n=2. We consider a magnetic Schrödinger operator L W , q in Ω and show how to recover the boundary values of the tangential component of the vector potential W from the Dirichlet to Neumann map for L W , q . We also consider a steady state heat equation with convection term Δ+2W·∇ and recover the boundary values of the convection term W from the Dirichlet to Neumann map. Our method is constructive and gives a stability result at the boundary.


Communications in Partial Differential Equations | 1997

Uniqueness in the inverse conductivity problem for nonsmooth conductivities in two dimensions

Russell M. Brown; Gunther Uhlmann

Let R 2 be a bounded domain with Lipschitz boundary and let : ! R be a function which is measurable and bounded away from zero and innnity. We consider the divergence form elliptic operator


Journal of Inverse and Ill-posed Problems | 2001

Recovering the conductivity at the boundary from the Dirichlet to Neumann map: a pointwise result

Russell M. Brown

Abstract - A formula is given for recovering the boundary values of the coefficient γ of an elliptic operator, divγ∇, from the Dirichlet to Neumann map. The main point is that one may recover γ without any a priori smoothness assumptions. The formula allows one to recover the value of γ pointwise.


Transactions of the American Mathematical Society | 2009

MIXED BOUNDARY VALUE PROBLEMS FOR THE STOKES SYSTEM

Russell M. Brown; Irina Mitrea; Marius Mitrea; M. Wright

We prove the well-posedness of the mixed problem for the Stokes system in a class of Lipschitz domains in ℝ n , n ≥ 3. The strategy is to reduce the original problem to a boundary integral equation, and we establish certain new Rellich-type estimates which imply that the intervening boundary integral operator is semi-Fredholm. We then prove that its index is zero by performing a homotopic deformation of it onto an operator related to the Lame system, which has recently been shown to be invertible.


Transactions of the American Mathematical Society | 1989

Area integral estimates for caloric functions

Russell M. Brown

We study the relationship between the area integral and the para- bolic maximal function of solutions to the heat equation in domains whose boundary satisfies a ( 5,1 ) mixed Lipschitz condition. Our main result states that the area integral and the parabolic maximal function are equivalent in LP(p), 0 < p < oo. The measure p. must satisfy Muckenhoupts /loo- condition with respect to caloric measure. We also give a Fatou theorem which shows that the existence of parabolic limits is a .e. (with respect to caloric measure) equivalent to the finiteness of the area integral.


Mathematische Annalen | 2008

The mixed problem in L p for some two-dimensional Lipschitz domains

Loredana Lanzani; Luca Capogna; Russell M. Brown

AbstractWe consider the mixed problem,


Transactions of the American Mathematical Society | 2012

The mixed problem in Lipschitz domains with general decompositions of the boundary

Justin L. Taylor; Katharine Ott; Russell M. Brown


Potential Analysis | 2013

The Mixed Problem for the Laplacian in Lipschitz Domains

Katharine Ott; Russell M. Brown

\left\{ \begin{array}{ll} \Delta u = 0 \quad & {\rm in }\, \Omega\\ \frac{\partial u }{\partial \nu} = f_N \quad & {\rm on }\, {\rm N} \\ u = f_D \quad & {\rm on}\,D \end{array} \right.


Journal of Nonlinear Science | 2001

Estimates for the Scattering Map Associated with a Two-Dimensional First-Order System

Russell M. Brown


Communications in Partial Differential Equations | 2013

The Green function for elliptic systems in two dimensions

Justin L. Taylor; Seick Kim; Russell M. Brown

in a class of Lipschitz graph domains in two dimensions with Lipschitz constant at most 1. We suppose the Dirichlet data, fD, has one derivative in Lp(D) of the boundary and the Neumann data, fN, is in Lp(N). We find a p0 > 1 so that for p in an interval (1, p0), we may find a unique solution to the mixed problem and the gradient of the solution lies in Lp.

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