2013
DOI: 10.1016/j.jmaa.2012.08.038
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Weak convergence analysis of the linear implicit Euler method for semilinear stochastic partial differential equations with additive noise

Abstract: a b s t r a c tIn this paper, we analyze the weak error of a semi-discretization in time by the linear implicit Euler method for semilinear stochastic partial differential equations (SPDEs) with additive noise. The main result reveals how the weak order depends on the regularity of noise and that the order of weak convergence is twice that of strong convergence. In particular, the linear implicit Euler method for SPDEs driven by trace class noise achieves an almost optimal order 1 − ϵ for arbitrarily small ϵ >… Show more

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Cited by 54 publications
(57 citation statements)
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“…Results related to (40) can, e.g., be found in Debussche [ (40) for all δ 1 , δ k ∈ (− 1 /2, 0], k ∈ {1, 2} without the constraint that δ 1 + δ 2 > − 1 /2 but under the additional assumption (2). Moreover, very roughly speaking, Lemma 3.3 in [50] establishes (40) for all δ 1 , δ k ∈ (−1, 0], k ∈ {1, 2} with the constraint that δ 1 + δ 2 > −1 in the case of additive noise. Note that condition (2) is obviously satisfied in the case of additive noise.…”
Section: Regularity Properties For Solutions Of Infinite Dimensional mentioning
confidence: 98%
See 1 more Smart Citation
“…Results related to (40) can, e.g., be found in Debussche [ (40) for all δ 1 , δ k ∈ (− 1 /2, 0], k ∈ {1, 2} without the constraint that δ 1 + δ 2 > − 1 /2 but under the additional assumption (2). Moreover, very roughly speaking, Lemma 3.3 in [50] establishes (40) for all δ 1 , δ k ∈ (−1, 0], k ∈ {1, 2} with the constraint that δ 1 + δ 2 > −1 in the case of additive noise. Note that condition (2) is obviously satisfied in the case of additive noise.…”
Section: Regularity Properties For Solutions Of Infinite Dimensional mentioning
confidence: 98%
“…Strong convergence rates for (temporal, spatial, and noise) numerical approximations for SEEs of the form (1) are well understood. Weak convergence rates for numerical approximations of SEEs of the form (1) have been investigated for about two decades; cf., e.g., [45,24,18,20,22,25,19,32,21,35,36,33,50,34,6,48,4,5,7,49]. Except for Debussche & De Bouard [18], Debussche [19], and Andersson & Larsson [5], all of the above mentioned references assume, beside further assumptions, that the considered SEE is driven by additive noise.…”
Section: Introductionmentioning
confidence: 99%
“…These tools have also been used in [28] to treat the time-discretization in a slightly more-general setting, and in [1] where discretization in space with a finite element method is studied. Basically, the two ingredients are the following:…”
Section: Introductionmentioning
confidence: 99%
“…for all t n = nh ≤ T , where C(u 0 , φ, T ) is independent of n, h. The weak order of accuracy (7) has been analyzed in [14] for (6) applied to the heat equation in the case F = 0 and in [12] in the semilinear case; see also [39] for the case of colored noise in dimension d > 1 and [23] where different techniques are used. Concerning the approximation of the invariant distribution of the heat equation, it is proved in [4] that for d = 1 and Q = I, one has for all time t n , similarly to (5), the exponential convergence property…”
Section: Introductionmentioning
confidence: 99%