Session 25. Nonlocal Phenomena: Levy processes and related operators

Weak convergence of finite element approximations of linear stochastic evolution equations with additive Lévy noise

Felix Lindner, Technische Universität Kaiserslautern, Germany
The talk is based on a joint work with Mihály Kovács (University of Otago, New Zealand) and René L. Schilling (TU Dresden, Germany).
We consider linear stochastic evolution equations of the form \[\mathrm dX(t)+AX(t) $\,$ \mathrm dt=B $\,$ \mathrm dZ(t),\quad t\in[0,T],\quad X(0)=X_0,\] where the solution process \(X\) takes values in a Hilbert space \(H\), \(-A\) is the generator of a strongly continuous operator semigroup on \(H\), \(B\) is an \(H\)-valued linear and bounded operator, and \(Z\) is an infinite dimensional Lévy process. For instance, the stochastic heat equation and the stochastic wave equation with additive Lévy noise can be written in this abstract form. Given an approximation \(\tilde X(T)\) of \(X(T)\), we are interested in estimating the weak error \(\big|\mathbb E \big(G(\tilde X(T))-G(X(T))\big)\big|\) for suitable test functions \(G:H\to\mathbb R\). We use It{\^o}'s formula and the backward Kolmogorov equations associated to certain auxiliary processes to derive a general error representation formula. The formula is then applied to spatially semidiscrete finite element methods for the stochastic heat equation and the stochastic wave equation. Explicit rates of convergence are obtained, depending on the type of the considered equation, the assumptions on \(Z\) and \(G\), and the order of the finite element method. The rates of weak and strong convergence are compared.
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