TheoremBase

The Gaussian Sobolev Space of the Noise Gradient

Defines the Gaussian Sobolev space Da1,2\mathbb{D}^{1,2}_a as the set of FF in L2(γc)L^2(\gamma_c) that are L2L^2-limits of bounded C1C^1 cylindrical functions whose noise gradients form a Cauchy sequence, and defines the noise gradient of such FF as the limit of those gradients, which does not depend on the approximating sequence.

Statement

In the setting of Gaussian Analysis Relative to a Diagonal Gaussian Reference Measure with Noise Weights: Standing Notation, with FCb1(X)\mathcal{F}C^{1}_{b}(X) and the noise gradients ∇aF\nabla_{a}F of Gaussian Analysis Relative to a Diagonal Gaussian Reference Measure with Noise Weights: Standing Notation §cylindrical, whose classes lie in L2(γc)L^{2}(\gamma_{c}) by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §square-integrable and in L2(γc;Xa)L^{2}(\gamma_{c};X^{a}) by The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradient respectively, and are again written FF and ∇aF\nabla_{a}F; L2(γc;Xa)L^{2}(\gamma_{c};X^{a}) is a real Hilbert space, with inner product ⟨⋅,⋅⟩γc\langle\cdot,\cdot\rangle_{\gamma_{c}} and norm ∥⋅∥γc\lVert\cdot\rVert_{\gamma_{c}}, by Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields.

1. (The Gaussian Sobolev space) Da1,2\mathbb{D}^{1,2}_{a} is the set of those F∈L2(γc)F\in L^{2}(\gamma_{c}) for which there is a sequence (Fj)j∈N(F_{j})_{j\in\mathbb{N}} in FCb1(X)\mathcal{F}C^{1}_{b}(X) such that (∥Fj−F∥2)j∈N(\lVert F_{j}-F\rVert_{2})_{j\in\mathbb{N}} converges to 00 and (∇aFj)j∈N(\nabla_{a}F_{j})_{j\in\mathbb{N}} is a Cauchy sequence in L2(γc;Xa)L^{2}(\gamma_{c};X^{a}); such a sequence approximates FF.

2. (The noise gradient) For F∈Da1,2F\in\mathbb{D}^{1,2}_{a} and an approximating sequence (Fj)(F_{j}), the Cauchy sequence (∇aFj)(\nabla_{a}F_{j}) converges in the complete space L2(γc;Xa)L^{2}(\gamma_{c};X^{a}), and its limit, the noise gradient ∇aF\nabla_{a}F of FF, does not depend on the approximating sequence: for a second approximating sequence (Fj′)(F'_{j}) with ∇aFj′→G′\nabla_{a}F'_{j}\to G' and ∇aFj→G\nabla_{a}F_{j}\to G, the functions Fj−Fj′F_{j}-F'_{j} lie in FCb1(X)\mathcal{F}C^{1}_{b}(X) by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §linear and satisfy ∥Fj−Fj′∥2≤∥Fj−F∥2+∥F−Fj′∥2→0\lVert F_{j}-F'_{j}\rVert_{2}\le\lVert F_{j}-F\rVert_{2}+\lVert F-F'_{j}\rVert_{2}\to0, and ∇a(Fj−Fj′)=∇aFj−∇aFj′→G−G′\nabla_{a}(F_{j}-F'_{j})=\nabla_{a}F_{j}-\nabla_{a}F'_{j}\to G-G'. Indeed, the noise gradient is the finite sum displayed in The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradient, and if FjF_{j}, Fj′F'_{j} and Fj−Fj′F_{j}-F'_{j} have representations (n,ψ)(n,\psi), (n′,ψ′)(n',\psi') and (m,χ)(m,\chi), all three sums may be taken up to k≤max⁡(n,n′,m)k\le\max(n,n',m) by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §partial; and the partial derivatives ∂k\partial_{k} are linear: if φ,φ′:X→R\varphi,\varphi':X\to\mathbb{R} are differentiable at x∈Xx\in X, then for z∈Xz\in X the number (φ−φ′)(x+z)−(φ−φ′)(x)−⟨Dφ(x)−Dφ′(x),z⟩(\varphi-\varphi')(x+z)-(\varphi-\varphi')(x)-\langle D\varphi(x)-D\varphi'(x),z\rangle is the difference of the two remainders φ(x+z)−φ(x)−⟨Dφ(x),z⟩\varphi(x+z)-\varphi(x)-\langle D\varphi(x),z\rangle and φ′(x+z)−φ′(x)−⟨Dφ′(x),z⟩\varphi'(x+z)-\varphi'(x)-\langle D\varphi'(x),z\rangle of Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space §differentiable, so, given a positive ε\varepsilon, it is at most ε∣z∣\varepsilon|z| in absolute value whenever ∣z∣|z| is less than both radii provided there for φ\varphi and for φ′\varphi' with ε/2\varepsilon/2 in place of ε\varepsilon; hence φ−φ′\varphi-\varphi' is differentiable at xx with gradient D(φ−φ′)(x)=Dφ(x)−Dφ′(x)D(\varphi-\varphi')(x)=D\varphi(x)-D\varphi'(x) by Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space §gradient, and since the partial derivatives of Partial Derivatives along an Orthonormal Basis of a Function Differentiable on a Hilbert Space §partial are the coordinates of the gradient, ∂k(φ−φ′)=∂kφ−∂kφ′\partial_{k}(\varphi-\varphi')=\partial_{k}\varphi-\partial_{k}\varphi' for functions differentiable on XX, as FjF_{j} and Fj′F'_{j} are by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §gradient. So G=G′G=G' by Gaussian Integration by Parts for Products of Cylindrical Functions, and Closability of the Noise Gradient in the Gaussian Lebesgue Space §closable. The noise gradient depends only on the class FF, since approximating sequences are constrained only through ∥Fj−F∥2\lVert F_{j}-F\rVert_{2}. For F∈FCb1(X)F\in\mathcal{F}C^{1}_{b}(X) the constant sequence approximates FF, so F∈Da1,2F\in\mathbb{D}^{1,2}_{a} and this noise gradient is the class of the noise gradient of The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradient.

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