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Integrals of Bounded C2C^2 Cylindrical Functions are Noise Intrinsic Test Functions with the Noise Gradient as Gradient

The integral of a bounded C2C^2 cylindrical function against a measure is a noise intrinsic test function on the noise Wasserstein space, and its gradient along noise couplings is the noise gradient of the function.

Statement

In the setting of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation, let Pρa\mathcal{P}^{a}_{\rho} be the set of The Measures Noise-Connected to the Reference Measure §space. Let n∈Nn\in\mathbb{N}, let f∈Cb2(Rn)f\in C^{2}_{b}(\mathbb{R}^{n}), the set of Bounded Twice Continuously Differentiable Functions with Bounded First and Second Partial Derivatives on Euclidean Space §bounded with q=nq=n, and let φ=f∘pn\varphi=f\circ p_{n}, a bounded C2C^{2} cylindrical function and hence a bounded C1C^{1} cylindrical function by Noise Gradients of Bounded C^2 Cylindrical Functions Are Dense in the Noise Tangent Space §inclusion. For μ∈P(X)\mu\in\mathcal{P}(X) the function φ\varphi is integrable with respect to μ\mu 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 the class of its noise gradient ∇aφ\nabla_{a}\varphi in L2(μ;Xa)L^{2}(\mu;X^{a}), again written ∇aφ\nabla_{a}\varphi, lies in the noise tangent space TμaT^{a}_{\mu} by Noise Gradients of Bounded C^2 Cylindrical Functions Are Dense in the Noise Tangent Space §inclusion. Let Uφ:Pρa→RU_{\varphi}:\mathcal{P}^{a}_{\rho}\to\mathbb{R} be the function

Uφ(μ)=∫Xφ dμ.U_{\varphi}(\mu)=\int_{X}\varphi\,d\mu .

Noise intrinsic test functions and the gradient along noise couplings ∇Uφ(μ)\nabla U_{\varphi}(\mu) are those of those definitions.

1. (Test function) For every subset Q⊆PρaQ\subseteq\mathcal{P}^{a}_{\rho}, UφU_{\varphi} is a noise intrinsic test function on QQ.

2. (Gradient) For every μ∈Pρa\mu\in\mathcal{P}^{a}_{\rho}, UφU_{\varphi} is differentiable along noise couplings at μ\mu and ∇Uφ(μ)=∇aφ\nabla U_{\varphi}(\mu)=\nabla_{a}\varphi in L2(μ;Xa)L^{2}(\mu;X^{a}).

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