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Proof of The Lift of the Second Moment: a Quadratic Function of Class C2C^2 with Gradient 2X and Translation Laplacian 2d

lemmalem:second-moment-lift-2026a
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· 8,022 chars · 34 deps · depth 27 Reason: Goal 3B: proof of lem:second-moment-lift-2026a.

The lift is the squared norm, a scaled squared distance to the origin, so its gradient and Hessian are read off the Hilbert-space quadratic lemma; along translations the squared norm expands into a constant, a linear function of the shift and the squared Euclidean norm of the shift, whose Laplacian at the origin is 2d.

Proof

Each result cited is universally quantified over the data in its own statement. Write L2L^{2} for L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}), a real Hilbert space with the differential calculus of Real Hilbert Spaces: Series, Products, Orthonormal Bases and Differential Calculus §calculus in force by The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §space, and 0L20_{L^{2}} for its zero vector; the identities of Elementary Identities in a Real Inner Product Space are in force for it by Real Hilbert Spaces: Standing Notation and Background §background. The natural number dd is read in R\mathbb{R} through the canonical map ι\iota of The Canonical Map from the Natural Numbers to a Field, as in the statement. Two identities are in play: II is the identity form on L2L^{2} of Real Hilbert Spaces: Standing Notation and Background §forms, while IdI_{d} in Claim 3 is the identity matrix of size dd.

Claim 1. For XL2X\in L^{2}, U(X)=u(L(X))=M2(L(X))U(X)=u(\mathcal{L}(X))=M_{2}(\mathcal{L}(X)) by The Lift of a Function on the Wasserstein Space to the Space of Square-Integrable Random Vectors §lift, and M2(L(X))=XL22M_{2}(\mathcal{L}(X))=\lVert X\rVert_{L^{2}}^{2} by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §law.

Claim 2. Let q:L2Rq:L^{2}\to\mathbb{R} be given by q(X)=22X0L2L22q(X)=\tfrac{2}{2}\lVert X-0_{L^{2}}\rVert_{L^{2}}^{2}. By Affine and Quadratic Functions on a Real Hilbert Space are of Class C2C^2 §quadratic, applied to the Hilbert space L2L^{2} with α=2\alpha=2 and y0=0L2y_{0}=0_{L^{2}}, the function qq belongs to C2(L2)C^{2}(L^{2}) with Dq(X)=2(X0L2)Dq(X)=2(X-0_{L^{2}}) and D2q(X)=2ID^{2}q(X)=2I for every XL2X\in L^{2}. Since 22=1\tfrac{2}{2}=1 in the field R\mathbb{R} and X0L2=XX-0_{L^{2}}=X by the axioms of the vector space L2L^{2}, we have q(X)=XL22=U(X)q(X)=\lVert X\rVert_{L^{2}}^{2}=U(X) for every XX by claim 1, that is, q=Uq=U. Hence UC2(L2)U\in C^{2}(L^{2}), DU(X)=2XDU(X)=2X and D2U(X)=2ID^{2}U(X)=2I. A function of class C2C^{2} is of class C1C^{1} by The Classes C1C^1 and C2C^2 on an Open Subset of a Real Inner Product Space §c2, so uu is continuously LL-differentiable by L-Differentiability of a Function on the Wasserstein Space via the Fréchet Derivative of Its Lift §c1; a function of class C1C^{1} is differentiable on L2L^{2} by The Classes C1C^1 and C2C^2 on an Open Subset of a Real Inner Product Space §c1, so uu is LL-differentiable with LL-gradient DU(X)=2XDU(X)=2X at XX by L-Differentiability of a Function on the Wasserstein Space via the Fréchet Derivative of Its Lift §differentiable.

Claim 3. Fix XL2X\in L^{2} and let ϕX:RdR\phi_{X}:\mathbb{R}^{d}\to\mathbb{R}, ϕX(a)=U(X+ca)\phi_{X}(a)=U(X+c_{a}), be the function of The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors. By claim 1 and Elementary Identities in a Real Inner Product Space §expansion,

ϕX(a)=X+caL22=XL22+2X,caL2+caL22=κ+2(a)+q0(a),\phi_{X}(a)=\lVert X+c_{a}\rVert_{L^{2}}^{2}=\lVert X\rVert_{L^{2}}^{2}+2\langle X,c_{a}\rangle_{L^{2}}+\lVert c_{a}\rVert_{L^{2}}^{2}=\kappa+2\ell(a)+q_{0}(a),

where κ=XL22\kappa=\lVert X\rVert_{L^{2}}^{2}, (a)=X,caL2\ell(a)=\langle X,c_{a}\rangle_{L^{2}} and q0(a)=a2q_{0}(a)=\lVert a\rVert^{2}, the last equality using caL2=a\lVert c_{a}\rVert_{L^{2}}=\lVert a\rVert from The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §constants. We treat the three summands in turn; Rd\mathbb{R}^{d} is open by claim 1 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous, and partial derivatives, the classes CkC^{k} and smoothness are those of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives.

The constant. The constant function with value κ\kappa is smooth on Rd\mathbb{R}^{d} by claim 2 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, hence of class C2C^{2} by Smooth Map on a Euclidean Open Set; and every partial derivative of a constant function exists and vanishes at every point, since its difference quotients in Partial Derivative on a Euclidean Open Set are all 00.

The linear term. For a,bRda,b\in\mathbb{R}^{d} and tRt\in\mathbb{R} the constant map with value a+ba+b is the pointwise sum of the constant maps with values aa and bb, and the constant map with value tata is tt times the constant map with value aa; hence ca+b=ca+cbc_{a+b}=c_{a}+c_{b} and cta=tcac_{ta}=t\,c_{a} by the operations on classes of The Space of Square-Integrable Random Vectors §classes, and therefore (a+b)=(a)+(b)\ell(a+b)=\ell(a)+\ell(b) and (ta)=t(a)\ell(ta)=t\,\ell(a) by Elementary Identities in a Real Inner Product Space §bilinear. Fix i[d]i\in[d] and let eiRde_{i}\in\mathbb{R}^{d} be the point with iith component 11 and every other component 00 (claim 2 of Euclidean Points as Tuples of Real Numbers). For aRda\in\mathbb{R}^{d} and hRh\in\mathbb{R}, the point with iith component ai+ha_{i}+h and kkth component aka_{k} for kik\ne i is a+heia+he_{i}, by claim 1 of Euclidean Points as Tuples of Real Numbers together with Sum of Points of Rn\mathbb{R}^n and Scalar Multiple of a Point of Rn\mathbb{R}^n. Hence for h0h\ne0

(a+hei)(a)h=(a)+h(ei)(a)h=(ei),\frac{\ell(a+he_{i})-\ell(a)}{h}=\frac{\ell(a)+h\,\ell(e_{i})-\ell(a)}{h}=\ell(e_{i}),

so the partial derivative of \ell with respect to the iith variable exists at every aa with value (ei)\ell(e_{i}) (Partial Derivative on a Euclidean Open Set, with any δ\delta); that is, i\partial_{i}\ell is the constant function with value (ei)\ell(e_{i}), which is smooth by claim 2 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, hence of class C1C^{1} by Smooth Map on a Euclidean Open Set and continuous at every point by claim 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous. The function \ell itself is continuous at every point: by The Cauchy-Schwarz Inequality in a Real Inner Product Space and The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §constants, (a)(b)=(ab)=X,cabL2XL2ab|\ell(a)-\ell(b)|=|\ell(a-b)|=|\langle X,c_{a-b}\rangle_{L^{2}}|\le\lVert X\rVert_{L^{2}}\lVert a-b\rVert, so given ε>0\varepsilon>0 the choice δ=ε/(XL2+1)\delta=\varepsilon/(\lVert X\rVert_{L^{2}}+1) gives (a)(b)<ε|\ell(a)-\ell(b)|<\varepsilon whenever ab<δ\lVert a-b\rVert<\delta (claim 10 of Elementary Order Arithmetic in an Ordered Field, and XL2<XL2+1\lVert X\rVert_{L^{2}}<\lVert X\rVert_{L^{2}}+1), which is continuity at bb relative to Rd\mathbb{R}^{d} in the sense of Continuous Map Between Metric Spaces for the metrics dEd_{E} and dRd_{\mathbb{R}} (Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n claim 2), hence continuity in the Euclidean sense by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions. Therefore \ell is of class C1C^{1} by clause 1 of C^k Maps on a Euclidean Open Set, and since each i\partial_{i}\ell is of class C1C^{1}, \ell is of class C2C^{2} by clause 2 there, with ji=0\partial_{j}\partial_{i}\ell=0 for all i,j[d]i,j\in[d] by the constant case above.

The quadratic term. By claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, q0(a)=a0Rd2=dE(a,0Rd)2q_{0}(a)=\lVert a-0_{\mathbb{R}^{d}}\rVert^{2}=d_{E}(a,0_{\mathbb{R}^{d}})^{2}, where a0Rd=aa-0_{\mathbb{R}^{d}}=a by Euclidean Space Rn\mathbb{R}^n is a Real Vector Space. So A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian, applied with its open set taken to be Rd\mathbb{R}^{d}, with c=1c=1 and the point 0Rd0_{\mathbb{R}^{d}}, shows that q0q_{0} is of class C2C^{2} on Rd\mathbb{R}^{d} (claim 2 there) with Hessian matrix D2q0(a)=2IdD^{2}q_{0}(a)=2I_{d} at every aa (claim 3 there). By Hessian Matrix of a C^2 Function, Scalar Multiple of a Real Matrix and Identity Matrix, the diagonal entries give iiq0(a)=(2Id)ii=21=2\partial_{i}\partial_{i}q_{0}(a)=(2I_{d})_{ii}=2\cdot1=2 for every i[d]i\in[d] and every aa.

Assembly. By claims 2 and 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, ϕX=κ+2+q0\phi_{X}=\kappa+2\ell+q_{0} is of class C2C^{2} on Rd\mathbb{R}^{d}, so UU is twice continuously differentiable along translations at XX by The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §translations, and, XX being arbitrary, on the whole space by The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §on-space. By claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set applied twice, for every i[d]i\in[d] and every aa,

iϕX(a)=0+2(ei)+iq0(a),iiϕX(a)=0+0+iiq0(a)=2,\partial_{i}\phi_{X}(a)=0+2\,\ell(e_{i})+\partial_{i}q_{0}(a),\qquad\partial_{i}\partial_{i}\phi_{X}(a)=0+0+\partial_{i}\partial_{i}q_{0}(a)=2,

the partial derivatives of the constants 00, 2(ei)2\ell(e_{i}) vanishing by the constant case. Hence, by The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §laplacian and The Laplacian of a Twice Continuously Differentiable Function §laplacian,

ΔtrU(X)=ΔϕX(0Rd)=i=1diiϕX(0Rd)=i=1d2=2i=1d1=2ι(d),\Delta_{\mathrm{tr}}U(X)=\Delta\phi_{X}(0_{\mathbb{R}^{d}})=\sum_{i=1}^{d}\partial_{i}\partial_{i}\phi_{X}(0_{\mathbb{R}^{d}})=\sum_{i=1}^{d}2=2\sum_{i=1}^{d}1=2\,\iota(d),

the last two steps by claim 3 of Properties of Finite Sums and The Canonical Map from the Natural Numbers to a Field. This is the claim, 2d2d denoting 2ι(d)2\,\iota(d).

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