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Feynman-Kac propagators and viscosity solutions
Authors:Archil Gulisashvili  Jan A. Van Casteren
Affiliation:(1) Department of Mathematics, Ohio University, Athens, Ohio 45701, USA;(2) Department of Mathematics and Computer Science, University of Antwerp (UA), Middelheimlaan 1, 2020 Antwerp, Belgium
Abstract:The aim of this paper is to study viscosity solutions to the following terminal value problem on [0, t] × E:
$$
left{ {begin{array}{*{20}l}
  {frac{{partial u}}
{{partial t}}(tau ,x) + [A(tau )u(tau )](x) - V(tau ,x)u(tau ,x) = 0} hfill 
  {u(t,x) = f(x),} hfill 
 end{array} } right.
$$
where E is a locally compact second countable Hausdorff topological space equipped with a reference measure mf isin Linfin(m), and V satisfies a Kato type condition. It is assumed that a transition probability density p is given, and the family of operators A(tau) is defined by
$$
A(tau )h(x) = mathop {lim }limits_{^{^{epsilon to 0 + } } } frac{{Y(tau + epsilon ,tau )h(x) - h(x)}}
{epsilon },
$$
where Y denotes the free backward propagator associated with p. It is shown in the paper that under some restrictions on p, V , tau0 isin [0,t), and x0 isin E, the backward Feynman-Kac propagator YV associated with p and V generates a viscosity solution to the terminal value problem above at the point (tau0, x0). Similar result holds in the case where the function V is replaced by a time-dependent family mgr of Borel measures on E.
Keywords:  KeywordHeading"  >Mathematics Subject Classifications (2000). Primary 47D08  49L25  Secondary 47D06  47D07
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