TheoremBase

Linearity of the Noise Gradient, and the Noise Tangent Space is a Closed Linear Subspace

The noise gradient is linear on bounded C1C^1 cylindrical functions, so the noise gradients form a linear subspace of the square-integrable noise fields and the noise tangent space, their closure, is a closed linear subspace.

Statement

In the setting of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation, let μ∈P(X)\mu\in\mathcal{P}(X). The set FCb1(X)\mathcal{F}C^{1}_{b}(X) of bounded C1C^{1} cylindrical functions, the noise gradient ∇aφ\nabla_{a}\varphi of φ∈FCb1(X)\varphi\in\mathcal{F}C^{1}_{b}(X), the set GμaG^{a}_{\mu} of The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradients and the noise tangent space TμaT^{a}_{\mu} are those of The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space, and L2(μ;Xa)L^{2}(\mu;X^{a}) is the real Hilbert space of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields. For φ,ψ∈FCb1(X)\varphi,\psi\in\mathcal{F}C^{1}_{b}(X) and s,t∈Rs,t\in\mathbb{R} the function sφ+tψs\varphi+t\psi belongs to 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, so that its noise gradient is defined; maps into XaX^{a} are added and multiplied by reals pointwise. Then the following hold.

1. (Linearity of the noise gradient) For all φ,ψ∈FCb1(X)\varphi,\psi\in\mathcal{F}C^{1}_{b}(X) and s,t∈Rs,t\in\mathbb{R},

∇a(sφ+tψ)=s ∇aφ+t ∇aψ.\nabla_{a}(s\varphi+t\psi)=s\,\nabla_{a}\varphi+t\,\nabla_{a}\psi .

2. (Linear subspaces) GμaG^{a}_{\mu} is a linear subspace of L2(μ;Xa)L^{2}(\mu;X^{a}), and TμaT^{a}_{\mu} is a closed linear subspace of L2(μ;Xa)L^{2}(\mu;X^{a}).

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