Abstract:In this work stochastic integration with respect to cylindrical Lévy processes with weak second moments is introduced. It is well known that a deterministic Hilbert-Schmidt operator radonifies a cylindrical random variable, i.e. it maps a cylindrical random variable to a classical Hilbert space valued random variable. Our approach is based on a generalisation of this result to the radonification of the cylindrical increments of a cylindrical Lévy process by random Hilbert-Schmidt operators. This generalisation… Show more
“…As a consequence of Douglas' theorem as stated in [38,Appendix A.4], compare also [41, Corollary C.0.6], the reproducing kernel Hilbert space of L has the alternative representation [38,Proposition 7.7]. The unique continuous extensions of the linear mappings U * 1 ∋ x → L(t), x ∈ L 2 (P), t 0, to the larger space U * determine a 2-cylindrical U-process in the sense of [35], compare also [1], [43], [44]. Remark 2.2.…”
We present an abstract framework to study weak convergence of numerical approximations of linear stochastic partial differential equations driven by additive Lévy noise. We first derive a representation formula for the error which we then apply to study space-time discretizations of the stochastic heat equation, a Volterra-type integro-differential equation, and the wave equation as examples. For twice continuously differentiable test functions with bounded second derivative (with an additional condition on the second derivative for the wave equation) the weak rate of convergence is found to be twice the strong rate. The results extend earlier work by two of the authors, as we consider general square-integrable infinite-dimensional Lévy processes and do not require boundedness of the test functions and their first derivative. Furthermore, the present framework is applicable to both hyperbolic and parabolic equations, and even to stochastic Volterra integro-differential equations.
“…As a consequence of Douglas' theorem as stated in [38,Appendix A.4], compare also [41, Corollary C.0.6], the reproducing kernel Hilbert space of L has the alternative representation [38,Proposition 7.7]. The unique continuous extensions of the linear mappings U * 1 ∋ x → L(t), x ∈ L 2 (P), t 0, to the larger space U * determine a 2-cylindrical U-process in the sense of [35], compare also [1], [43], [44]. Remark 2.2.…”
We present an abstract framework to study weak convergence of numerical approximations of linear stochastic partial differential equations driven by additive Lévy noise. We first derive a representation formula for the error which we then apply to study space-time discretizations of the stochastic heat equation, a Volterra-type integro-differential equation, and the wave equation as examples. For twice continuously differentiable test functions with bounded second derivative (with an additional condition on the second derivative for the wave equation) the weak rate of convergence is found to be twice the strong rate. The results extend earlier work by two of the authors, as we consider general square-integrable infinite-dimensional Lévy processes and do not require boundedness of the test functions and their first derivative. Furthermore, the present framework is applicable to both hyperbolic and parabolic equations, and even to stochastic Volterra integro-differential equations.
“…In Métivier and Pellaumail [15], the construction is extended to cylindrical local martingales. For the special case of a cylindrical Lévy process with finite weak second moments one can follow a classical Itô aproach to define the stochastic integral for random integrands; see Riedle [23].…”
A cylindrical Lévy process does not enjoy a cylindrical version of the semimartingale decomposition which results in the need to develop a completely novel approach to stochastic integration. In this work, we introduce a stochastic integral for random integrands with respect to cylindrical Lévy processes in Hilbert spaces. The space of admissible integrands consists of adapted stochastic processes with values in the space of Hilbert-Schmidt operators. Neither the integrands nor the integrator is required to satisfy any moment or boundedness condition. The integral process is characterised as an adapted, Hilbert space valued semi-martingale with càdlàg trajectories.
“…This refers to finding a mapping into a possibly larger space that transforms the cylindrical object into a bona fide one. A important theorem [26] states that if (M(t), t ≥ 0) is a cylindrical semimartingale in H, then there exists a Hilbert-Schmidt operator T on H and a semimartingale (N(t), t ≥ 0) so that the real-valued processes (M(t)(T * x), t ≥ 0) and ( N(t), x , t ≥ 0) are indistinguishable, for all x ∈ H. In Theorem 5.10 of [47], conditions are found for a suitable deterministic function f so that its cylindrical stochastic integral t 0 f (s)dL(s) has the property of stochastic integrability in that there exists a random variable I t such that for all u ∈ H, I t , u = t 0 f (s)dL(s) (u) (see also Corollary 4.4 in [46]). An alternative approach has been developed in a series of papers that focus on the specific class of cylindrical Lévy processes defined by (7.23), with the assumption that the L n 's are i.i.d.…”
We review the probabilistic properties of Ornstein-Uhlenbeck processes in Hilbert spaces driven by Lévy processes. The emphasis is on the different contexts in which these processes arise, such as stochastic partial differential equations, continuous-state branching processes, generalised Mehler semigroups and operator self-decomposable distributions. We also examine generalisations to the case where the driving noise is cylindrical.
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