TheoremBase

The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space

Defines the noise gradient of a bounded C1C^1 cylindrical function, a bounded measurable map into the noise space, and the noise tangent space at a probability measure as the closure of the noise gradients in the square-integrable noise fields.

Statement

In the setting of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation, let FCb1(X)\mathcal{F}C^{1}_{b}(X) be the set of bounded C1C^{1} cylindrical functions, with their representations. Every φ∈FCb1(X)\varphi\in\mathcal{F}C^{1}_{b}(X) is differentiable on XX 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, and for k∈Nk\in\mathbb{N}, ∂kφ\partial_{k}\varphi is its kk-th partial derivative. For μ∈P(X)\mu\in\mathcal{P}(X), 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, and measurability of maps into XaX^{a} is that fixed there.

1. (Noise gradient) Let φ∈FCb1(X)\varphi\in\mathcal{F}C^{1}_{b}(X) have a representation (n,ψ)(n,\psi). The noise gradient of φ\varphi is the map ∇aφ:X→Xa\nabla_{a}\varphi:X\to X^{a},

∇aφ(x)=∑k=1nak ∂kφ(x) ek(x∈X).\nabla_{a}\varphi(x)=\sum_{k=1}^{n}a_{k}\,\partial_{k}\varphi(x)\,e_{k}\qquad(x\in X).

It does not depend on the representation: 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, ∂kφ(x)=0\partial_{k}\varphi(x)=0 for k>nk>n and every x∈Xx\in X, so for a second representation (m,χ)(m,\chi) the sums over k≤nk\le n and over k≤mk\le m coincide. Its values lie in XaX^{a}, which is a linear subspace of XX by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §hilbert and contains each ek=ak−1/2fke_{k}=a_{k}^{-1/2}f_{k} by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §basis. By the orthonormality of (ek)k∈N(e_{k})_{k\in\mathbb{N}} the kk-th coordinate of ∇aφ(x)\nabla_{a}\varphi(x) is ak ∂kφ(x)a_{k}\,\partial_{k}\varphi(x) for k≤nk\le n and 00 for k>nk>n, so that, by The Noise Space of a Weight Sequence on a Hilbert Space with an Orthonormal Basis §inner-product,

∣∇aφ(x)∣a2=∑k=1nak (∂kφ(x))2(x∈X).|\nabla_{a}\varphi(x)|_{a}^{2}=\sum_{k=1}^{n}a_{k}\,\bigl(\partial_{k}\varphi(x)\bigr)^{2}\qquad(x\in X).

The coordinate function x↦ak ∂kφ(x)x\mapsto a_{k}\,\partial_{k}\varphi(x) is Borel for k≤nk\le n, ∂kφ\partial_{k}\varphi being Borel by Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §bounded-borel, and the coordinate function for k>nk>n, being constant 00, is Borel; so ∇aφ\nabla_{a}\varphi is measurable into XaX^{a} by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §measurable, and the function ∣∇aφ∣a2:X→R|\nabla_{a}\varphi|_{a}^{2}:X\to\mathbb{R}, the finite sum ∑k=1nak(∂kφ)2\sum_{k=1}^{n}a_{k}(\partial_{k}\varphi)^{2} of the display, is Borel and nonnegative by Measurable Maps into a Hilbert Space with an Orthonormal Basis: Norms, Inner Products and Linear Combinations, Synthesis from Coordinates, Square-Integrability, and Almost-Everywhere Equality §operations, applied with E=XaE=X^{a} and v=∇aφv=\nabla_{a}\varphi. By Bounded C^1 Cylindrical Functions: Linear Structure, the Gradient and the Partial Derivatives, Bounds and Integrability, and Density in the Square-Integrable Functions §bounded-borel there are also real numbers Bk≥0B_{k}\ge0 with ∣∂kφ(x)∣≤Bk|\partial_{k}\varphi(x)|\le B_{k} for k≤nk\le n and x∈Xx\in X, so the display gives ∣∇aφ(x)∣a2≤B|\nabla_{a}\varphi(x)|_{a}^{2}\le B for every x∈Xx\in X, with B=∑k=1nakBk2B=\sum_{k=1}^{n}a_{k}B_{k}^{2}. Hence for every μ∈P(X)\mu\in\mathcal{P}(X) the monotonicity of Linearity and Monotonicity of the Lebesgue Integral §nonnegative, applied with f=∣∇aφ∣a2f=|\nabla_{a}\varphi|_{a}^{2} and gg the constant function BB, gives ∫X∣∇aφ∣a2 dμ≤B μ(X)=B<∞\int_{X}|\nabla_{a}\varphi|_{a}^{2}\,d\mu\le B\,\mu(X)=B<\infty, and ∇aφ\nabla_{a}\varphi is square-integrable with respect to μ\mu in the sense of The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §space.

2. (Noise gradients of cylindrical functions) For μ∈P(X)\mu\in\mathcal{P}(X), GμaG^{a}_{\mu} denotes the set of the classes in L2(μ;Xa)L^{2}(\mu;X^{a}) of the noise gradients ∇aφ\nabla_{a}\varphi of the functions φ∈FCb1(X)\varphi\in\mathcal{F}C^{1}_{b}(X).

3. (Noise tangent space) For μ∈P(X)\mu\in\mathcal{P}(X), the noise tangent space at μ\mu is the closure of GμaG^{a}_{\mu} in L2(μ;Xa)L^{2}(\mu;X^{a}),

Tμa=Gμa‾.T^{a}_{\mu}=\overline{G^{a}_{\mu}} .

Citations

Loading…

Dependencies

Loading…

Related

0 relations

Curated associations between results. These are editable and subjective — they do not replace the dependency graph, which is derived from the references in the text.

No relations recorded yet.

Comments

Log in to comment.

Loading…