TheoremBase

The field is synthesised from the square-summable coordinates ak1/2a_k^{1/2} zetakzeta_k, and its pairings with noise gradients reduce to finitely many coordinate inner products, which the defining identity of the relative score turns into the Ornstein-Uhlenbeck functional. The lift of the score of the rescaled head has coordinates given by the projections of the score components, so Pythagoras and the head Fisher information give the approximation identity, and closedness of the noise tangent space gives tangency.

Proof

Each result cited is universally quantified over the data in its own statement. The notation of A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation is in force. The space L2(μ;Xa)L^{2}(\mu;X^{a}) is that of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields, that is, the space of The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis on (X,B(X),μ)(X,\mathcal{B}(X),\mu) with E=XaE=X^{a} and the orthonormal basis (fk)k∈N(f_{k})_{k\in\mathbb{N}}, fk=ak1/2ekf_{k}=a_{k}^{1/2}e_{k} (Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §noise-space); its scalar space L2(μ)=L2(X,B(X),μ)L^{2}(\mu)=L^{2}(X,\mathcal{B}(X),\mu) is the space of The Relative Score with Respect to a Diagonal Gaussian Measure on a Hilbert Space in which the ζk\zeta_{k} lie. For v∈L2(μ;Xa)v\in L^{2}(\mu;X^{a}) and k∈Nk\in\mathbb{N}, vk∈L2(μ)v_{k}\in L^{2}(\mu) is the coordinate of vv along fkf_{k} (The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates), the class of x↦⟨v(x),fk⟩ax\mapsto\langle v(x),f_{k}\rangle_{a} for a representative vv. Every aka_{k} is positive (Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §weights, Weight Sequences and the Weighted Fisher Information Relative to a Diagonal Gaussian Measure on a Hilbert Space §weights), and for y∈Xay\in X^{a} one has ⟨y,fk⟩a=ak−1/2⟨y,ek⟩\langle y,f_{k}\rangle_{a}=a_{k}^{-1/2}\langle y,e_{k}\rangle by The Noise Space is a Real Hilbert Space: Orthonormal Basis, Continuous Embedding, Partial Sums, Closed Balls and Borel Measurability §basis.

Step 1 (Claim 1). Since μ\mu has finite Fisher information relative to γc\gamma_{c} with weights aa, the series ∑k=1∞ak∥ζk∥L2(μ)2\sum_{k=1}^{\infty}a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2} converges, with sum Ia(μ ∣ γc)\mathcal{I}_{a}(\mu\,|\,\gamma_{c}) (Weight Sequences and the Weighted Fisher Information Relative to a Diagonal Gaussian Measure on a Hilbert Space §information). For each kk, ak1/2ζk∈L2(μ)a_{k}^{1/2}\zeta_{k}\in L^{2}(\mu) and ∥ak1/2ζk∥L2(μ)2=ak∥ζk∥L2(μ)2\lVert a_{k}^{1/2}\zeta_{k}\rVert_{L^{2}(\mu)}^{2}=a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2} by the homogeneity of the norm, so the series ∑k=1∞∥ak1/2ζk∥L2(μ)2\sum_{k=1}^{\infty}\lVert a_{k}^{1/2}\zeta_{k}\rVert_{L^{2}(\mu)}^{2} converges, and The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §synthesis provides exactly one Zμa∈L2(μ;Xa)Z^{a}_{\mu}\in L^{2}(\mu;X^{a}) with (Zμa)k=ak1/2ζk(Z^{a}_{\mu})_{k}=a_{k}^{1/2}\zeta_{k} for every k∈Nk\in\mathbb{N}. By The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates,

∥Zμa∥μ2=∑k=1∞∥ak1/2ζk∥L2(μ)2=∑k=1∞ak∥ζk∥L2(μ)2=Ia(μ ∣ γc).\lVert Z^{a}_{\mu}\rVert_{\mu}^{2}=\sum_{k=1}^{\infty}\lVert a_{k}^{1/2}\zeta_{k}\rVert_{L^{2}(\mu)}^{2}=\sum_{k=1}^{\infty}a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2}=\mathcal{I}_{a}(\mu\,|\,\gamma_{c}).

This proves claim 1.

Step 2 (Coordinates of a noise gradient). Let n∈Nn\in\mathbb{N}, g∈Cb1(Rn)g\in C^{1}_{b}(\mathbb{R}^{n}) and φ=g∘pn\varphi=g\circ p_{n}, a bounded C1C^{1} cylindrical function with representation (n,g)(n,g) (Bounded C^1 Cylindrical Functions on a Hilbert Space with an Orthonormal Basis §cylindrical, Bounded C^1 Cylindrical Functions on a Hilbert Space with an Orthonormal Basis §representation). Let x∈Xx\in X. By The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradient, ∇aφ(x)∈Xa\nabla_{a}\varphi(x)\in X^{a} and ⟨∇aφ(x),ek⟩\langle\nabla_{a}\varphi(x),e_{k}\rangle equals ak ∂kφ(x)a_{k}\,\partial_{k}\varphi(x) for k≤nk\le n and 00 for k>nk>n; and ∂kφ=(∂kg)∘pn\partial_{k}\varphi=(\partial_{k}g)\circ p_{n} for k≤nk\le n 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. Hence the coordinate of ∇aφ(x)\nabla_{a}\varphi(x) along fkf_{k} is ak−1/2ak ∂kg(pn(x))=ak1/2 ∂kg(pn(x))a_{k}^{-1/2}a_{k}\,\partial_{k}g(p_{n}(x))=a_{k}^{1/2}\,\partial_{k}g(p_{n}(x)) for k≤nk\le n, and 00 for k>nk>n. The map ∇aφ\nabla_{a}\varphi is square-integrable with respect to μ\mu (The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §gradient) and represents its own class, so (∇aφ)k(\nabla_{a}\varphi)_{k} is the class of ak1/2(∂kg)∘pna_{k}^{1/2}(\partial_{k}g)\circ p_{n} for k∈[n]k\in[n] and the zero vector of L2(μ)L^{2}(\mu) for k>nk>n.

Step 3 (Claim 2). In the situation of Step 2, The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates gives ⟨Zμa,∇aφ⟩μ=∑k=1∞⟨(Zμa)k,(∇aφ)k⟩L2(μ)\langle Z^{a}_{\mu},\nabla_{a}\varphi\rangle_{\mu}=\sum_{k=1}^{\infty}\langle(Z^{a}_{\mu})_{k},(\nabla_{a}\varphi)_{k}\rangle_{L^{2}(\mu)}. The terms with k>nk>n vanish, the second argument being the zero vector, so the partial sums (Series of Real Numbers §partial-sums) are constant from the index nn on and the sum (Series of Real Numbers §convergent) is the nnth partial sum. By Steps 1 and 2 and the bilinearity of the inner product of L2(μ)L^{2}(\mu),

⟨Zμa,∇a(g∘pn)⟩μ=∑k=1n⟨ak1/2ζk,ak1/2(∂kg)∘pn⟩L2(μ)=∑k=1nak ⟨ζk,(∂kg)∘pn⟩L2(μ).\langle Z^{a}_{\mu},\nabla_{a}(g\circ p_{n})\rangle_{\mu}=\sum_{k=1}^{n}\bigl\langle a_{k}^{1/2}\zeta_{k},a_{k}^{1/2}(\partial_{k}g)\circ p_{n}\bigr\rangle_{L^{2}(\mu)}=\sum_{k=1}^{n}a_{k}\,\langle\zeta_{k},(\partial_{k}g)\circ p_{n}\rangle_{L^{2}(\mu)} .

This proves claim 2.

Step 4 (Claim 3). Let n∈Nn\in\mathbb{N} and g∈Cb2(Rn)g\in C^{2}_{b}(\mathbb{R}^{n}); then g∈Cb1(Rn)g\in C^{1}_{b}(\mathbb{R}^{n}), as noted in the statement, so claim 2 applies to gg. Let k∈[n]k\in[n]. As recorded in the preamble of The Noise Ornstein-Uhlenbeck Functional of a Probability Measure at a Bounded C^2 Function of Finitely Many Coordinates, ∂kg∈Cb1(Rn)\partial_{k}g\in C^{1}_{b}(\mathbb{R}^{n}), so (∂kg)∘pn(\partial_{k}g)\circ p_{n} is a bounded C1C^{1} cylindrical function with representation (n,∂kg)(n,\partial_{k}g), and 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 its kkth partial derivative is (∂k∂kg)∘pn(\partial_{k}\partial_{k}g)\circ p_{n}. The defining identity of the relative score (The Relative Score with Respect to a Diagonal Gaussian Measure on a Hilbert Space §score), applied with this cylindrical function, gives

⟨ζk,(∂kg)∘pn⟩L2(μ)=∫X(xkck ∂kg(pn(x))−∂k∂kg(pn(x)))μ(dx),\langle\zeta_{k},(\partial_{k}g)\circ p_{n}\rangle_{L^{2}(\mu)}=\int_{X}\Bigl(\frac{x_{k}}{c_{k}}\,\partial_{k}g(p_{n}(x))-\partial_{k}\partial_{k}g(p_{n}(x))\Bigr)\mu(dx),

the numbers ckc_{k} being those of the variance sequence cc of A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation §gaussian in both places. Multiplying by aka_{k} and summing over k∈[n]k\in[n], claim 2 and The Noise Ornstein-Uhlenbeck Functional of a Probability Measure at a Bounded C^2 Function of Finitely Many Coordinates §functional give ⟨Zμa,∇a(g∘pn)⟩μ=Lμa(g)\langle Z^{a}_{\mu},\nabla_{a}(g\circ p_{n})\rangle_{\mu}=L^{a}_{\mu}(g). This proves claim 3.

Step 5 (Claim 4). Let n∈Nn\in\mathbb{N}. By The Relative Score of the Rescaled Head: Projections of the Score, the Ornstein-Uhlenbeck Functional of the Head, and the Converse under Bounded Head Fisher Information §head-score, μ~n\tilde{\mu}_{n} has finite Fisher information relative to γ~n\tilde{\gamma}_{n}; write ζ~=ζμ~nc~(n)\tilde{\zeta}=\zeta^{\tilde{c}^{(n)}}_{\tilde{\mu}_{n}}, an element of Tμ~n⊆L2(μ~n;Rn)T_{\tilde{\mu}_{n}}\subseteq L^{2}(\tilde{\mu}_{n};\mathbb{R}^{n}) (Finite Fisher Information Relative to a Diagonal Gaussian Measure: the Ornstein-Uhlenbeck Functional, the Relative Score and the Relative Fisher Information §score), and let η=(η1,…,ηn)\eta=(\eta_{1},\dots,\eta_{n}) be a representative of ζ~\tilde{\zeta}, a Borel map with ∫∥η∥2 dμ~n<∞\int\lVert\eta\rVert^{2}\,d\tilde{\mu}_{n}<\infty (Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §l2mu). Each ηk\eta_{k} is a Borel representative of the component ζ~k\tilde{\zeta}_{k} of ζ~\tilde{\zeta} (preamble of Finite Fisher Information Relative to a Diagonal Gaussian Measure on Euclidean Space as Componentwise Integration by Parts against Bounded C^1 Functions, as fixed in A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation §euclidean). By Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §lift, Λnη\Lambda_{n}\eta takes values in XaX^{a}, is square-integrable with respect to μ\mu, and represents Λnζ~\Lambda_{n}\tilde{\zeta}. For x∈Xx\in X, Λnη(x)=∑j=1naj1/2ηj(rn(x)) ej\Lambda_{n}\eta(x)=\sum_{j=1}^{n}a_{j}^{1/2}\eta_{j}(r_{n}(x))\,e_{j}, so by the linearity of the inner product of XX and the orthonormality of (ej)(e_{j}), ⟨Λnη(x),ek⟩\langle\Lambda_{n}\eta(x),e_{k}\rangle is ak1/2ηk(rn(x))a_{k}^{1/2}\eta_{k}(r_{n}(x)) for k≤nk\le n and 00 for k>nk>n; hence the coordinate of Λnη(x)\Lambda_{n}\eta(x) along fkf_{k} is ηk(rn(x))\eta_{k}(r_{n}(x)) for k≤nk\le n and 00 for k>nk>n. By The Relative Score of the Rescaled Head: Projections of the Score, the Ornstein-Uhlenbeck Functional of the Head, and the Converse under Bounded Head Fisher Information §head-score, applied with the Borel representative ηk\eta_{k} of ζ~k\tilde{\zeta}_{k}, Πnζk\Pi_{n}\zeta_{k} is the class of ak−1/2(ηk∘rn)a_{k}^{-1/2}(\eta_{k}\circ r_{n}), so the class of ηk∘rn\eta_{k}\circ r_{n} is ak1/2Πnζka_{k}^{1/2}\Pi_{n}\zeta_{k}. Therefore (Λnζ~)k=ak1/2Πnζk(\Lambda_{n}\tilde{\zeta})_{k}=a_{k}^{1/2}\Pi_{n}\zeta_{k} for k∈[n]k\in[n] and (Λnζ~)k(\Lambda_{n}\tilde{\zeta})_{k} is the zero vector for k>nk>n, and by the linearity of coordinates (The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates) the element W=Zμa−Λnζ~W=Z^{a}_{\mu}-\Lambda_{n}\tilde{\zeta} has

Wk=ak1/2(ζk−Πnζk)(k∈[n]),Wk=ak1/2ζk(k>n).W_{k}=a_{k}^{1/2}(\zeta_{k}-\Pi_{n}\zeta_{k})\quad(k\in[n]),\qquad W_{k}=a_{k}^{1/2}\zeta_{k}\quad(k>n).

The subspace VnV_{n} is a closed linear subspace of the real Hilbert space L2(μ)L^{2}(\mu) (Relative Scores of the Finite-Dimensional Projections on a Hilbert Space: Orthogonal Projections of the Score, and the Weighted Fisher Information as the Limit of Its Cutoffs §subspace), so Orthogonal Projection onto a Closed Linear Subspace of a Real Hilbert Space §pythagoras gives ∥ζk∥L2(μ)2=∥Πnζk∥L2(μ)2+∥ζk−Πnζk∥L2(μ)2\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2}=\lVert\Pi_{n}\zeta_{k}\rVert_{L^{2}(\mu)}^{2}+\lVert\zeta_{k}-\Pi_{n}\zeta_{k}\rVert_{L^{2}(\mu)}^{2}. Hence ∥Wk∥L2(μ)2=ak∥ζk∥L2(μ)2−ak∥Πnζk∥L2(μ)2\lVert W_{k}\rVert_{L^{2}(\mu)}^{2}=a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2}-a_{k}\lVert\Pi_{n}\zeta_{k}\rVert_{L^{2}(\mu)}^{2} for k∈[n]k\in[n] and ∥Wk∥L2(μ)2=ak∥ζk∥L2(μ)2\lVert W_{k}\rVert_{L^{2}(\mu)}^{2}=a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2} for k>nk>n. Let sN=∑k=1Nak∥ζk∥L2(μ)2s_{N}=\sum_{k=1}^{N}a_{k}\lVert\zeta_{k}\rVert_{L^{2}(\mu)}^{2} and tN=∑k=1N∥Wk∥L2(μ)2t_{N}=\sum_{k=1}^{N}\lVert W_{k}\rVert_{L^{2}(\mu)}^{2} be the partial sums (Series of Real Numbers §partial-sums). For N≥nN\ge n, splitting the finite sums at nn and using The Relative Score of the Rescaled Head: Projections of the Score, the Ornstein-Uhlenbeck Functional of the Head, and the Converse under Bounded Head Fisher Information §head-fisher,

tN=sN−∑k=1nak∥Πnζk∥L2(μ)2=sN−I(μ~n ∣ γ~n).t_{N}=s_{N}-\sum_{k=1}^{n}a_{k}\lVert\Pi_{n}\zeta_{k}\rVert_{L^{2}(\mu)}^{2}=s_{N}-\mathcal{I}(\tilde{\mu}_{n}\,|\,\tilde{\gamma}_{n}).

As N→∞N\to\infty, sN→Ia(μ ∣ γc)s_{N}\to\mathcal{I}_{a}(\mu\,|\,\gamma_{c}) by Step 1 and Series of Real Numbers §convergent, and tN→∥W∥μ2t_{N}\to\lVert W\rVert_{\mu}^{2} by The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates; so

∥Zμa−Λnζ~∥μ2=Ia(μ ∣ γc)−I(μ~n ∣ γ~n).\bigl\lVert Z^{a}_{\mu}-\Lambda_{n}\tilde{\zeta}\bigr\rVert_{\mu}^{2}=\mathcal{I}_{a}(\mu\,|\,\gamma_{c})-\mathcal{I}(\tilde{\mu}_{n}\,|\,\tilde{\gamma}_{n}).

By The Relative Score of the Rescaled Head: Projections of the Score, the Ornstein-Uhlenbeck Functional of the Head, and the Converse under Bounded Head Fisher Information §head-fisher-convergence, I(μ~n ∣ γ~n)→Ia(μ ∣ γc)\mathcal{I}(\tilde{\mu}_{n}\,|\,\tilde{\gamma}_{n})\to\mathcal{I}_{a}(\mu\,|\,\gamma_{c}) as n→∞n\to\infty, so the right-hand side tends to 00. This proves claim 4.

Step 6 (Claim 5). For n∈Nn\in\mathbb{N}, the relative score ζμ~nc~(n)\zeta^{\tilde{c}^{(n)}}_{\tilde{\mu}_{n}} lies in Tμ~nT_{\tilde{\mu}_{n}} (Finite Fisher Information Relative to a Diagonal Gaussian Measure: the Ornstein-Uhlenbeck Functional, the Relative Score and the Relative Fisher Information §score), so its lift vn=Λnζμ~nc~(n)v_{n}=\Lambda_{n}\zeta^{\tilde{c}^{(n)}}_{\tilde{\mu}_{n}} lies in TμaT^{a}_{\mu} by Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §tangent. By claim 4, the distance ∥Zμa−vn∥μ\lVert Z^{a}_{\mu}-v_{n}\rVert_{\mu} is the nonnegative square root of a sequence of nonnegative numbers tending to 00, so it tends to 00; that is, the sequence (vn)n∈N(v_{n})_{n\in\mathbb{N}} in TμaT^{a}_{\mu} converges to ZμaZ^{a}_{\mu} in the metric space L2(μ;Xa)L^{2}(\mu;X^{a}) (Real Hilbert Space §topology). By Sequential Characterization of the Closure in a Metric Space, ZμaZ^{a}_{\mu} lies in the closure of TμaT^{a}_{\mu}. Now TμaT^{a}_{\mu} is the closure of GμaG^{a}_{\mu} (The Noise Gradient of a Cylindrical Function and the Noise Tangent Space at a Probability Measure on a Hilbert Space §tangent), which is closed by claim 2 of The Closure is the Smallest Closed Superset, and so equals its own closure by claim 4 there. Hence Zμa∈TμaZ^{a}_{\mu}\in T^{a}_{\mu}, which proves claim 5.

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