1991
DOI: 10.1515/9783110858389
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Dirichlet Forms and Analysis on Wiener Space

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Cited by 457 publications
(594 citation statements)
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“…It is determined by X φ dΓ(u, u) = E(u, φu) − 1 2 E(u 2 , φ) and called energy measure; see also [11]. The energy measure satisfies the Leibniz rule, dΓ(u · v, w) = udΓ(v, w) + vdΓ(u, w), as well as the chain rule…”
Section: Assumptions and Basic Propertiesmentioning
confidence: 99%
“…It is determined by X φ dΓ(u, u) = E(u, φu) − 1 2 E(u 2 , φ) and called energy measure; see also [11]. The energy measure satisfies the Leibniz rule, dΓ(u · v, w) = udΓ(v, w) + vdΓ(u, w), as well as the chain rule…”
Section: Assumptions and Basic Propertiesmentioning
confidence: 99%
“…We refer to [Kat66,Kat80] for a detailed description of the general theory and to [BH91] [FOT94] for the theory of Dirichlet forms. Throughout we assume that X is a locally compact σ-compact metric space and µ a positive Radon measure with supp µ = X.…”
Section: Preliminariesmentioning
confidence: 99%
“…If ξ ∈ B(E) + then E ξ is a Markovian form which satisfies the bounds 0 ≤ E ξ (ϕ) ≤ ξ ∞ E(ϕ) for all ϕ ∈ B(E) (see [BH91], Proposition I.4.1.1). Therefore the quadratic form E ξ extends by continuity to a Markovian form on D(E) although the identity (5) is not necessarily valid for the extension.…”
Section: IImentioning
confidence: 99%
“…An alternative method that we will use here is based on potential theory (see Albeverio [1], Bouleau and Hirsch [5] and Fukushima et al [17]) suggested by Bouleau [6]. We assume that the uncertainties are small random variables added to the true values of the parameters.…”
Section: Introductionmentioning
confidence: 99%