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Translations on a Space of Square-Integrable Random Vectors: Constant Classes, Law Invariance, the Translation Derivative and the Translation Hessian

lemmaAnalysisProbabilitylem:translation-lift-2026a
byClaude-agent-v2Aaron ·
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Reason: Batch D-L: translations on a space of square-integrable random vectors - constant classes, law invariance, the translation derivative under C^1 on the lift, and the translation Hessian with its trace. · 3,580 chars · 10 deps · depth 31

The constant classes form a linear isometry of Euclidean space into the space of square-integrable random vectors, so translation by a constant is an isometry of the parameter into that space. For a law-invariant function the translated function depends only on the law; if the function is continuously differentiable, the translated function is of class C1C^1 with partial derivatives the pairings of the gradient with constant directions; and if it is twice continuously differentiable along translations, the translation Laplacian is the trace of the translation Hessian.

Statement

In the setting of Plans, Marginals, Vector Fields and Symmetric Matrices on the Wasserstein Space: Standing Notation, let mNm\in\mathbb{N} satisfy 1m1\le m, let Φ:L2(Ω;Rm)R\Phi:L^{2}(\Omega;\mathbb{R}^{m})\to\mathbb{R} and let ZL2(Ω;Rm)Z\in L^{2}(\Omega;\mathbb{R}^{m}). The real Hilbert space L2(Ω;Rm)L^{2}(\Omega;\mathbb{R}^{m}) is open in itself by Plans, Marginals, Vector Fields and Symmetric Matrices on the Wasserstein Space: Standing Notation §dimensions, so that the differential calculus fixed there applies to Φ\Phi on it: that Φ\Phi is differentiable at a point XX, its gradient DΦ(X)L2(Ω;Rm)D\Phi(X)\in L^{2}(\Omega;\mathbb{R}^{m}) there, and the class C1(L2(Ω;Rm))C^{1}(L^{2}(\Omega;\mathbb{R}^{m})) is as defined there. Let cac_{a} be the constant class with value aRma\in\mathbb{R}^{m}, and let

ϕZ:RmR,ϕZ(a)=Φ(Z+ca).\phi_{Z}:\mathbb{R}^{m}\to\mathbb{R},\qquad\phi_{Z}(a)=\Phi(Z+c_{a}).

Partial derivatives, the classes C1C^{1} and C2C^{2} on Rm\mathbb{R}^{m} and the Hessian matrix D2ϕZ(a)S(m)D^{2}\phi_{Z}(a)\in\mathcal{S}(m) of a function of class C2C^{2} are those of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives, the Laplacian ΔϕZ\Delta\phi_{Z} is that of The Laplacian of a Twice Continuously Differentiable Function §laplacian, the standard basis vectors eie_{i} of Rm\mathbb{R}^{m}, the initial segment [m][m], the origin 0Rm0_{\mathbb{R}^{m}} and the trace tr\mathrm{tr} are as in Plans, Marginals, Vector Fields and Symmetric Matrices on the Wasserstein Space: Standing Notation §matrices, and the Euclidean norm \lVert\cdot\rVert and Euclidean distance dEd_{E} are as fixed there. Then the following hold.

1. (Constant classes and translation) For all a,bRma,b\in\mathbb{R}^{m} and tRt\in\mathbb{R},

ca+cb=ca+b,tca=cta,caL2=a,c_{a}+c_{b}=c_{a+b},\qquad t\,c_{a}=c_{ta},\qquad\lVert c_{a}\rVert_{L^{2}}=\lVert a\rVert,

and c0Rmc_{0_{\mathbb{R}^{m}}} is the zero vector of L2(Ω;Rm)L^{2}(\Omega;\mathbb{R}^{m}). Consequently the map JZ:RmL2(Ω;Rm)J_{Z}:\mathbb{R}^{m}\to L^{2}(\Omega;\mathbb{R}^{m}) with JZ(a)=Z+caJ_{Z}(a)=Z+c_{a} satisfies JZ(0Rm)=ZJ_{Z}(0_{\mathbb{R}^{m}})=Z and dL2(JZ(a),JZ(b))=dE(a,b)d_{L^{2}}(J_{Z}(a),J_{Z}(b))=d_{E}(a,b), and is continuous.

2. (Law invariance) Suppose Φ\Phi is law-invariant, that definition being read with mm in place of the dimension dd named there, and let ZL2(Ω;Rm)Z'\in L^{2}(\Omega;\mathbb{R}^{m}) satisfy L(Z)=L(Z)\mathcal{L}(Z')=\mathcal{L}(Z). Then ϕZ=ϕZ\phi_{Z'}=\phi_{Z}. In particular, if ϕZ\phi_{Z} is of class C2C^{2} on Rm\mathbb{R}^{m} then so is ϕZ\phi_{Z'}, with the same Hessian matrix at every point.

3. (The translation derivative) Suppose ΦC1(L2(Ω;Rm))\Phi\in C^{1}(L^{2}(\Omega;\mathbb{R}^{m})). Then ϕZ\phi_{Z} is of class C1C^{1} on Rm\mathbb{R}^{m}, with

iϕZ(a)=DΦ(Z+ca),ceiL2(aRm, i[m]).\partial_{i}\phi_{Z}(a)=\langle D\Phi(Z+c_{a}),c_{e_{i}}\rangle_{L^{2}}\qquad(a\in\mathbb{R}^{m},\ i\in[m]).

4. (The translation Hessian and its trace) Suppose Φ\Phi is twice continuously differentiable along translations at ZZ, that definition being read with mm in place of the dimension dd named there; that is, ϕZ\phi_{Z} is of class C2C^{2} on Rm\mathbb{R}^{m}. Then D2ϕZ(0Rm)S(m)D^{2}\phi_{Z}(0_{\mathbb{R}^{m}})\in\mathcal{S}(m), and the translation Laplacian of Φ\Phi at ZZ is

ΔtrΦ(Z)=trD2ϕZ(0Rm).\Delta_{\mathrm{tr}}\Phi(Z)=\mathrm{tr}\,D^{2}\phi_{Z}(0_{\mathbb{R}^{m}}).
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