Abstract:In this article we introduce a theory of integration for deterministic, operator-valued integrands with respect to cylindrical Lévy processes in separable Banach spaces. Here, a cylindrical Lévy process is understood in the classical framework of cylindrical random variables and cylindrical measures, and thus, it can be considered as a natural generalisation of cylindrical Wiener processes or white noises. Depending on the underlying Banach space, we provide necessary and/or sufficient conditions for a functio… Show more
“…Furthermore, Lemma 4.3 implies for every β ∈ Ê and v ∈ V that E exp(iβ ∆ n (t), v )| F n,kn = exp (t − t n,kn )S(βΦ * n,kn v) P -a.s., (5.52) where S : U → denotes the cylindrical Lévy symbol of L. The set {Φ * n,kn (ω)v : n ∈ AE} is uniformly bounded as Φ n,kn (ω) is in the closure of {Ψ(t)(ω) : t ∈ [0, T ]} for every ω ∈ Ω and the closure of the latter is compact by Proposition 1.1 in [9]. As S maps bounded sets to bounded sets by Lemma 3.2 in [24], we conclude from (5.51) and (5.52) that lim n→∞ E exp(iβ ∆ n (t), v )| F n,kn = 0 P -a.s. for every β ∈ Ê.…”
Section: The Stochastic Integralmentioning
confidence: 99%
“…Some specific examples and their constructions of cylindrical Lévy processes are presented in the work [24] by Riedle. Linear and semi-linear stochastic partial differential equations perturbed by an additive noise which is modelled by various but specific examples of cylindrical Lévy processes can be found for example in the works Brzeźniak and Zabczyk [3], Peszat and Zabczyk [20], and Priola and Zabczyk [21]. However, modelling an arbitrary perturbation of a general stochastic partial differential equations beyond the purely additive case requires a theory of stochastic integration of random integrands with respect to cylindrical Lévy processes.…”
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.
“…Furthermore, Lemma 4.3 implies for every β ∈ Ê and v ∈ V that E exp(iβ ∆ n (t), v )| F n,kn = exp (t − t n,kn )S(βΦ * n,kn v) P -a.s., (5.52) where S : U → denotes the cylindrical Lévy symbol of L. The set {Φ * n,kn (ω)v : n ∈ AE} is uniformly bounded as Φ n,kn (ω) is in the closure of {Ψ(t)(ω) : t ∈ [0, T ]} for every ω ∈ Ω and the closure of the latter is compact by Proposition 1.1 in [9]. As S maps bounded sets to bounded sets by Lemma 3.2 in [24], we conclude from (5.51) and (5.52) that lim n→∞ E exp(iβ ∆ n (t), v )| F n,kn = 0 P -a.s. for every β ∈ Ê.…”
Section: The Stochastic Integralmentioning
confidence: 99%
“…Some specific examples and their constructions of cylindrical Lévy processes are presented in the work [24] by Riedle. Linear and semi-linear stochastic partial differential equations perturbed by an additive noise which is modelled by various but specific examples of cylindrical Lévy processes can be found for example in the works Brzeźniak and Zabczyk [3], Peszat and Zabczyk [20], and Priola and Zabczyk [21]. However, modelling an arbitrary perturbation of a general stochastic partial differential equations beyond the purely additive case requires a theory of stochastic integration of random integrands with respect to cylindrical Lévy processes.…”
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.
“…In the very recent paper [19], Riedle systemically researched OU processes driven by cylindrical Lévy processes in infinite dimensional space. His Theorem 8.4 obtains a result similar to Theorem 2.3 (2).…”
In this paper we first obtain a necessary condition for H -càdlàg modification and H -weakly càdlàg modification of generalized Ornstein-Uhlenbeck processes with Lévy noises in Hilbert spaces H . Then we give a necessary and sufficient condition for the H -càdlàg modification and H -weakly càdlàg modification of Ornstein-Uhlenbeck processes driven by cylindrical α-semistable processes. Secondly, we investigate the properties of cylindrical càdlàg modification and V -cylindrical càdlàg modification. Applying the obtained results to diagonal Ornstein-Uhlenbeck processes with α-stable noises, we show a necessary and sufficient condition for cylindrical càdlàg modification and V -cylindrical càdlàg modification in the symmetric case for α ∈ (0, 1) and give a sufficient condition in the general case for α ∈ (0, 2). Some examples illustrate the relations among the concepts of various càdlàg modifications.
“…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.…”
“…, X(t)a n ) is a Lévy process in R n . As shown in Lemma 4.2 of [47], the representation (7.23) gives a specific class of examples of this more general notion when we identify L(t) therein with the mapping which sends each a ∈ H to the random variable ∞ n=1 β n L n (t) e n , a , where the β n 's are chosen to ensure the series converges for all t ≥ 0. In particular, we obtain a cylindrical Lévy process in the case where 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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