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Proof of The Lift of a Linear Functional of the Measure: Integrability, L-Gradient, Lipschitz Gradient Map and Translation Laplacian

lemmalem:linear-functional-lift-2026a
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Pointwise Taylor bounds for f with uniform constants are integrated against the law: the first-order bound gives linear growth and integrability, the second-order bound gives the Fréchet expansion of the lift with an explicit remainder, the Lipschitz bound on the gradient transfers to the gradient map, and the translation Laplacian is computed by differentiation under the expectation and dominated convergence.

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}); 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, and we write dd for ι(d)\iota(d) inside real expressions, as in the statement. Elements of L2L^{2} are handled through representatives, again written with the same letter, as the convention of The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §space allows; the operations on classes are those of The Space of Square-Integrable Random Vectors §classes. For x,hRdx,h\in\mathbb{R}^{d} the segment {x+τh:0τ1}\{x+\tau h:0\le\tau\le1\} lies in Rd\mathbb{R}^{d}, which is open by claim 1 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous, and h=dE(x,x+h)=h|h|=d_{E}(x,x+h)=\lVert h\rVert in the notation of Multivariate Taylor Expansion with Uniform Second-Order Remainder by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. Since ff is of class C2C^{2}, each if\partial_{i}f is of class C1C^{1} with partial derivatives jif\partial_{j}\partial_{i}f, by clause 2 of C^k Maps on a Euclidean Open Set. We record four pointwise bounds, valid for all x,hRdx,h\in\mathbb{R}^{d}.

(T1) f(x+h)f(x)dM1h|f(x+h)-f(x)|\le\sqrt{d}\,M_{1}\lVert h\rVert, by claim (i) of Multivariate Taylor Expansion with Uniform Second-Order Remainder applied to ff with the bound M1M_{1}.

(T2) f(x+h)f(x)Df(x)h12dM2h2\bigl|f(x+h)-f(x)-Df(x)\cdot h\bigr|\le\tfrac12\,d\,M_{2}\lVert h\rVert^{2}, by claim (ii) there applied to ff with the bound M2M_{2}, since i=1dif(x)hi=Df(x)h\sum_{i=1}^{d}\partial_{i}f(x)h_{i}=Df(x)\cdot h by Gradient of a Real-Valued Function on a Euclidean Open Set and Difference, Dot Product, and Orthogonality in Rn\mathbb{R}^n.

(T3) if(x+h)if(x)dM2h|\partial_{i}f(x+h)-\partial_{i}f(x)|\le\sqrt{d}\,M_{2}\lVert h\rVert for every i[d]i\in[d], by claim (i) there applied to if\partial_{i}f with the bound M2M_{2}.

(T4) Df(x+h)Df(x)dM2h\lVert Df(x+h)-Df(x)\rVert\le d\,M_{2}\lVert h\rVert. Indeed, by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, clause 1 of Difference, Dot Product, and Orthogonality in Rn\mathbb{R}^n and Gradient of a Real-Valued Function on a Euclidean Open Set, Df(x+h)Df(x)2=i=1d(if(x+h)if(x))2\lVert Df(x+h)-Df(x)\rVert^{2}=\sum_{i=1}^{d}(\partial_{i}f(x+h)-\partial_{i}f(x))^{2}; each summand is at most (dM2h)2=dM22h2(\sqrt{d}M_{2}\lVert h\rVert)^{2}=d\,M_{2}^{2}\lVert h\rVert^{2} by (T3), claim 1 of Nonnegativity of Squares in an Ordered Field and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field (the square root being that of Existence and Uniqueness of the Nonnegative Square Root); summing, by claims 2 and 5 of Properties of Finite Sums applied to the nonnegative differences, then claim 3 there and The Canonical Map from the Natural Numbers to a Field for the constant sum, Df(x+h)Df(x)2ddM22h2=(dM2h)2\lVert Df(x+h)-Df(x)\rVert^{2}\le d\cdot d\,M_{2}^{2}\lVert h\rVert^{2}=(d\,M_{2}\lVert h\rVert)^{2}, and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives (T4), both sides being nonnegative.

(G) Also, by (T1) with x=0Rdx=0_{\mathbb{R}^{d}} and claim 5 of Properties of the Absolute Value in an Ordered Field, for every xRdx\in\mathbb{R}^{d}

f(x)f(0Rd)+dM1xf(0Rd)+dM1+dM1x2,|f(x)|\le|f(0_{\mathbb{R}^{d}})|+\sqrt{d}\,M_{1}\lVert x\rVert\le|f(0_{\mathbb{R}^{d}})|+\sqrt{d}\,M_{1}+\sqrt{d}\,M_{1}\lVert x\rVert^{2},

the second step because x1+x2\lVert x\rVert\le1+\lVert x\rVert^{2}: if x1\lVert x\rVert\le1 this holds as 0x20\le\lVert x\rVert^{2} (claim 2 of Nonnegativity of Squares in an Ordered Field), and if 1<x1<\lVert x\rVert then x=x1<xx\lVert x\rVert=\lVert x\rVert\cdot1<\lVert x\rVert\cdot\lVert x\rVert by claim 10 of Elementary Order Arithmetic in an Ordered Field, so xx21+x2\lVert x\rVert\le\lVert x\rVert^{2}\le1+\lVert x\rVert^{2}; then multiply by the nonnegative dM1\sqrt{d}M_{1} (claim 5 of Elementary Arithmetic in an Ordered Field).

Claim 1. Let μP2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}), a probability measure on (Rd,B(Rd))(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d})) by The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §space and Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures. The function g(x)=f(0Rd)+dM1+dM1x2g(x)=|f(0_{\mathbb{R}^{d}})|+\sqrt{d}M_{1}+\sqrt{d}M_{1}\lVert x\rVert^{2} is integrable with respect to μ\mu: the constant is integrable by claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space (μ\mu being a Borel measure with μ(Rd)=1\mu(\mathbb{R}^{d})=1 by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures), the nonnegative Borel function xx2x\mapsto\lVert x\rVert^{2} (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs) has integral M2(μ)<M_{2}(\mu)<\infty by The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §moment and The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §space, hence is integrable by Integrable Function and the Lebesgue Integral (the two readings of its integral agreeing by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures), and linear combinations of integrable functions are integrable by claim 2 of Linearity and Monotonicity of the Lebesgue Integral. Since ff is Borel, f|f| is Borel by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and fg|f|\le g pointwise by (G); so fdμgdμ<\int|f|\,d\mu\le\int g\,d\mu<\infty by the monotonicity in claim 1 of Linearity and Monotonicity of the Lebesgue Integral, and ff is integrable with respect to μ\mu by Integrable Function and the Lebesgue Integral. Thus uu is defined. For XL2X\in L^{2} and a representative of it, L(X)P2(Rd)\mathcal{L}(X)\in\mathcal{P}_{2}(\mathbb{R}^{d}) by The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §law-map, so ff is integrable with respect to L(X)\mathcal{L}(X), whence fXf\circ X is integrable and E[fX]=fdL(X)=u(L(X))=U(X)\mathbb{E}[f\circ X]=\int f\,d\mathcal{L}(X)=u(\mathcal{L}(X))=U(X) by Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §expectation and The Lift of a Function on the Wasserstein Space to the Space of Square-Integrable Random Vectors §lift.

Claim 2. Square-integrability and the class. For every xRdx\in\mathbb{R}^{d}, Df(x)2=i=1dif(x)2i=1dM12=dM12\lVert Df(x)\rVert^{2}=\sum_{i=1}^{d}\partial_{i}f(x)^{2}\le\sum_{i=1}^{d}M_{1}^{2}=d\,M_{1}^{2}, by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, the hypothesis ifM1|\partial_{i}f|\le M_{1} with claim 1 of Nonnegativity of Squares in an Ordered Field and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, claims 2 and 5 of Properties of Finite Sums, and the constant sum as in (T4). Hence, for a random vector XX, E[DfX2]E[dM12]=dM12P(Ω)=dM12<\mathbb{E}[\lVert Df\circ X\rVert^{2}]\le\mathbb{E}[d\,M_{1}^{2}]=d\,M_{1}^{2}P(\Omega)=d\,M_{1}^{2}<\infty by the monotonicity and homogeneity in claim 1 of Linearity and Monotonicity of the Lebesgue Integral and The Integral of an Indicator Function is the Measure of the Set (the constant being dM121Ωd\,M_{1}^{2}\mathbf{1}_{\Omega}), so DfXDf\circ X is square-integrable by The Space of Square-Integrable Random Vectors §space. If XX' is another representative, P(X=X)=1P(X=X')=1 by The Space of Square-Integrable Random Vectors §classes; the event {DfX=DfX}\{Df\circ X=Df\circ X'\} (an event by Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §almost-sure) contains {X=X}\{X=X'\}, so it has probability 11 by the monotonicity of PP (claim 2 of Basic Properties of a Measure) and P(Ω)=1P(\Omega)=1, whence DfXDf\circ X and DfXDf\circ X' have the same class by Square-Integrable Random Vectors: Coordinates, Operations, Almost Sure Equality and the Mean-Square Form §almost-sure.

Differentiability. Fix XL2X\in L^{2} and let ZL2Z\in L^{2}, with representatives X,ZX,Z; then X+ZX+Z is a representative of the class X+ZX+Z. Applying (T2) at each ω\omega with x=X(ω)x=X(\omega) and h=Z(ω)h=Z(\omega),

f(X+Z)fX(DfX)Z12dM2Z2pointwise on Ω,\bigl|f\circ(X+Z)-f\circ X-(Df\circ X)\cdot Z\bigr|\le\tfrac12\,d\,M_{2}\lVert Z\rVert^{2}\qquad\text{pointwise on }\Omega,

where (DfX)Z(Df\circ X)\cdot Z and Z2\lVert Z\rVert^{2} are the random variables of Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §composition. The three random variables on the left are integrable: f(X+Z)f\circ(X+Z) and fXf\circ X by claim 1, and (DfX)Z(Df\circ X)\cdot Z by Square-Integrable Random Vectors: Coordinates, Operations, Almost Sure Equality and the Mean-Square Form §operations, with E[(DfX)Z]=DfX,ZL2\mathbb{E}[(Df\circ X)\cdot Z]=\langle Df\circ X,Z\rangle_{L^{2}} by The Space of Square-Integrable Random Vectors §inner-product; and E[Z2]=ZL22\mathbb{E}[\lVert Z\rVert^{2}]=\lVert Z\rVert_{L^{2}}^{2} by The Space of Square-Integrable Random Vectors §inner-product and Existence and Uniqueness of the Nonnegative Square Root. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral (linearity, |\int\cdot|\le\int|\cdot| and monotonicity, the absolute value of an integrable function being measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions and integrable by Integrable Function and the Lebesgue Integral), together with claim 1,

U(X+Z)U(X)DfX,ZL2E[f(X+Z)fX(DfX)Z]12dM2ZL22.\bigl|U(X+Z)-U(X)-\langle Df\circ X,Z\rangle_{L^{2}}\bigr|\le\mathbb{E}\bigl[\bigl|f\circ(X+Z)-f\circ X-(Df\circ X)\cdot Z\bigr|\bigr]\le\tfrac12\,d\,M_{2}\lVert Z\rVert_{L^{2}}^{2}.

Let ε>0\varepsilon>0. If dM2=0d\,M_{2}=0, the right-hand side is 0εZL20\le\varepsilon\lVert Z\rVert_{L^{2}} for every ZZ (claim 1 of Zero Products and Elementary Identities in a Field, ZL20\lVert Z\rVert_{L^{2}}\ge0 by Real Inner Product Space §norm). Otherwise M20M_{2}\ne0, so 0<M20<M_{2} as M2M_{2} is nonnegative, and dM2>0d\,M_{2}>0 by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field and claim 5 of Elementary Order Arithmetic in an Ordered Field; we put δ=2ε(dM2)1>0\delta=2\varepsilon\,(d\,M_{2})^{-1}>0 (claims 7 and 5 of Elementary Order Arithmetic in an Ordered Field); for ZL2<δ\lVert Z\rVert_{L^{2}}<\delta we get 12dM2ZL22=12dM2ZL2ZL212dM2δZL2=εZL2\tfrac12\,d\,M_{2}\lVert Z\rVert_{L^{2}}^{2}=\tfrac12\,d\,M_{2}\lVert Z\rVert_{L^{2}}\cdot\lVert Z\rVert_{L^{2}}\le\tfrac12\,d\,M_{2}\,\delta\,\lVert Z\rVert_{L^{2}}=\varepsilon\lVert Z\rVert_{L^{2}} by claim 5 of Elementary Arithmetic in an Ordered Field. In either case every ZZ with ZL2<δ\lVert Z\rVert_{L^{2}}<\delta (any δ>0\delta>0 in the first case) satisfies X+ZL2X+Z\in L^{2} and the inequality of Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space §differentiable with p=DfXp=Df\circ X; so UU is differentiable at XX with gradient DU(X)=DfXDU(X)=Df\circ X (Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space §gradient). As XX was arbitrary, UU is differentiable on L2L^{2} (Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space §on-set), that is, uu is LL-differentiable with LL-gradient DfXDf\circ X at XX by L-Differentiability of a Function on the Wasserstein Space via the Fréchet Derivative of Its Lift §differentiable.

Claim 3. Let X,YL2X,Y\in L^{2} with representatives X,YX,Y. By claim 2, DU(X)DU(Y)DU(X)-DU(Y) is the class of DfXDfYDf\circ X-Df\circ Y (The Space of Square-Integrable Random Vectors §classes and Square-Integrable Random Vectors: Coordinates, Operations, Almost Sure Equality and the Mean-Square Form §vector-space), and (T4) at each ω\omega with x=Y(ω)x=Y(\omega), h=X(ω)Y(ω)h=X(\omega)-Y(\omega) gives DfXDfYdM2XY\lVert Df\circ X-Df\circ Y\rVert\le d\,M_{2}\lVert X-Y\rVert pointwise, hence DfXDfY2d2M22XY2\lVert Df\circ X-Df\circ Y\rVert^{2}\le d^{2}M_{2}^{2}\lVert X-Y\rVert^{2} pointwise by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. Taking expectations (monotonicity and homogeneity in claim 1 of Linearity and Monotonicity of the Lebesgue Integral) and using The Space of Square-Integrable Random Vectors §inner-product with Existence and Uniqueness of the Nonnegative Square Root on both sides,

DU(X)DU(Y)L22d2M22XYL22=(dM2XYL2)2,\lVert DU(X)-DU(Y)\rVert_{L^{2}}^{2}\le d^{2}M_{2}^{2}\lVert X-Y\rVert_{L^{2}}^{2}=(d\,M_{2}\lVert X-Y\rVert_{L^{2}})^{2},

and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives the asserted inequality, both sides being nonnegative. The gradient map is therefore continuous on L2L^{2}: given YY and ε>0\varepsilon>0, δ=ε(dM2+1)1\delta=\varepsilon(d\,M_{2}+1)^{-1} gives DU(X)DU(Y)L2dM2XYL2<ε\lVert DU(X)-DU(Y)\rVert_{L^{2}}\le d\,M_{2}\lVert X-Y\rVert_{L^{2}}<\varepsilon whenever XYL2<δ\lVert X-Y\rVert_{L^{2}}<\delta (claim 5 of Elementary Arithmetic in an Ordered Field, claim 10 of Elementary Order Arithmetic in an Ordered Field and dM2<dM2+1d\,M_{2}<d\,M_{2}+1), which is Continuous Map Between Metric Spaces for the metric dL2d_{L^{2}}. Hence UC1(L2)U\in C^{1}(L^{2}) by The Classes C1C^1 and C2C^2 on an Open Subset of a Real Inner Product Space §c1, and uu is continuously LL-differentiable by L-Differentiability of a Function on the Wasserstein Space via the Fréchet Derivative of Its Lift §c1.

Claim 4. Fix XL2X\in L^{2} with a representative XX, and let 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. For aRda\in\mathbb{R}^{d} the map X+a:ωX(ω)+aX+a:\omega\mapsto X(\omega)+a is a representative of X+caX+c_{a} (The Space of Square-Integrable Random Vectors §classes, The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §constants), so by claim 1

ϕX(a)=E[f(X+a)](aRd).\phi_{X}(a)=\mathbb{E}[f\circ(X+a)]\qquad(a\in\mathbb{R}^{d}).

For i[d]i\in[d] let eiRde_{i}\in\mathbb{R}^{d} have iith component 11 and every other component 00; the point with iith component ai+ha_{i}+h and the other components those of aa is a+heia+he_{i}, since both points have the same components (claims 1 and 2 of Euclidean Points as Tuples of Real Numbers, the components of a+heia+he_{i} being ak+h(ei)ka_{k}+h(e_{i})_{k} by Sum of Points of Rn\mathbb{R}^n and Scalar Multiple of a Point of Rn\mathbb{R}^n).

Step A: first partial derivatives. Let g:RdRg:\mathbb{R}^{d}\to\mathbb{R} be of class C1C^{1} with igK|\partial_{i}g|\le K on Rd\mathbb{R}^{d} for every i[d]i\in[d] and some nonnegative KK, and suppose that g(X+b)g\circ(X+b) is integrable for every bRdb\in\mathbb{R}^{d}. Put ψ(a)=E[g(X+a)]\psi(a)=\mathbb{E}[g\circ(X+a)]. We show that for every aRda\in\mathbb{R}^{d} and i[d]i\in[d] the partial derivative iψ(a)\partial_{i}\psi(a) exists and equals E[ig(X+a)]\mathbb{E}[\partial_{i}g\circ(X+a)]. Let J=(1,1)J=(-1,1), an interval all of whose points are interior by An Open Interval is an Interval All of Whose Points Are Interior, and let F:J×ΩRF:J\times\Omega\to\mathbb{R}, F(t,ω)=g(X(ω)+a+tei)F(t,\omega)=g(X(\omega)+a+te_{i}). Condition (i) of Differentiation under the Integral Sign holds by hypothesis with b=a+teib=a+te_{i}. For (ii), fix ω\omega and put x=X(ω)+ax=X(\omega)+a: by claim 2 of Derivatives Along a Segment for C^1 Functions on a Euclidean Open Set with h=eih=e_{i}, the function tg(x+tei)t\mapsto g(x+te_{i}) is differentiable at every point tt of JJ with derivative k=1dkg(x+tei)(ei)k=ig(x+tei)\sum_{k=1}^{d}\partial_{k}g(x+te_{i})(e_{i})_{k}=\partial_{i}g(x+te_{i}), the sum having a single possibly nonzero summand (claim 7 of Properties of Finite Sums), so D1F(t,ω)=ig(X(ω)+a+tei)D_{1}F(t,\omega)=\partial_{i}g(X(\omega)+a+te_{i}). For (iii), D1F(t,ω)K|D_{1}F(t,\omega)|\le K, and the constant K1ΩK\mathbf{1}_{\Omega} is integrable on (Ω,F,P)(\Omega,\mathcal{F},P) with integral KK, by The Integral of an Indicator Function is the Measure of the Set, the homogeneity in claim 1 of Linearity and Monotonicity of the Lebesgue Integral and Integrable Function and the Lebesgue Integral. The theorem gives that tE[g(X+a+tei)]=ψ(a+tei)t\mapsto\mathbb{E}[g\circ(X+a+te_{i})]=\psi(a+te_{i}) is differentiable on JJ with derivative E[ig(X+a+tei)]\mathbb{E}[\partial_{i}g\circ(X+a+te_{i})] at tt; at t=0t=0 this reads: for every ε>0\varepsilon>0 there is δ>0\delta>0 such that every hh with 0<h<δ0<|h|<\delta and hJh\in J satisfies ψ(a+hei)ψ(a)hE[ig(X+a)]<ε\bigl|\frac{\psi(a+he_{i})-\psi(a)}{h}-\mathbb{E}[\partial_{i}g\circ(X+a)]\bigr|<\varepsilon (Derivative at an Interior Point). Taking δ1\delta\le1, the restriction hJh\in J is automatic, and since a+heia+he_{i} is the point with iith component ai+ha_{i}+h, this is exactly the statement of Partial Derivative on a Euclidean Open Set that iψ(a)\partial_{i}\psi(a) exists with value E[ig(X+a)]\mathbb{E}[\partial_{i}g\circ(X+a)].

Step B: continuity of the averaged functions. Let g:RdRg:\mathbb{R}^{d}\to\mathbb{R} be continuous at every point in the Euclidean sense and bounded by a nonnegative constant KK, and put ψ(a)=E[g(X+a)]\psi(a)=\mathbb{E}[g\circ(X+a)], defined since gg is Borel (claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions and Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps), so that g(X+a)g\circ(X+a) is a random variable by Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §composition, bounded by KK, hence integrable by the monotonicity and homogeneity in claim 1 of Linearity and Monotonicity of the Lebesgue Integral against the constant K1ΩK\mathbf{1}_{\Omega}, whose integral is KK by The Integral of an Indicator Function is the Measure of the Set. We show ψ\psi is continuous at every point in the Euclidean sense. By claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions and Continuity Between Metric Spaces is Equivalent to Sequential Continuity §criterion it suffices to show: if (am)mN(a_{m})_{m\in\mathbb{N}} converges to aa in (Rd,dE)(\mathbb{R}^{d},d_{E}) then ψ(am)ψ(a)\psi(a_{m})\to\psi(a). For each ω\omega, dE(X(ω)+am,X(ω)+a)=ama=dE(am,a)d_{E}(X(\omega)+a_{m},X(\omega)+a)=\lVert a_{m}-a\rVert=d_{E}(a_{m},a) by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, so X(ω)+amX(ω)+aX(\omega)+a_{m}\to X(\omega)+a in (Rd,dE)(\mathbb{R}^{d},d_{E}) (Convergent Sequence in a Metric Space), and g(X(ω)+am)g(X(ω)+a)g(X(\omega)+a_{m})\to g(X(\omega)+a) by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions and Continuity Between Metric Spaces is Equivalent to Sequential Continuity §sequential. The functions g(X+am)g\circ(X+a_{m}) are measurable and bounded by the integrable constant KK, so Dominated Convergence Theorem gives ψ(am)=g(X+am)dPg(X+a)dP=ψ(a)\psi(a_{m})=\int g\circ(X+a_{m})\,dP\to\int g\circ(X+a)\,dP=\psi(a).

Step C: assembly. By Step A with g=fg=f, K=M1K=M_{1} (integrability by claim 1), iϕX(a)=E[if(X+a)]\partial_{i}\phi_{X}(a)=\mathbb{E}[\partial_{i}f\circ(X+a)] for all aa and ii. By Step A with g=ifg=\partial_{i}f, K=M2K=M_{2} (of class C1C^{1} with partials jif\partial_{j}\partial_{i}f; if(X+b)\partial_{i}f\circ(X+b) integrable as in Step B, being bounded by M1M_{1}), jiϕX(a)=E[jif(X+a)]\partial_{j}\partial_{i}\phi_{X}(a)=\mathbb{E}[\partial_{j}\partial_{i}f\circ(X+a)] for all aa and i,ji,j. By Step B with g=ifg=\partial_{i}f, K=M1K=M_{1} and with g=jifg=\partial_{j}\partial_{i}f, K=M2K=M_{2} (continuous at every point by Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives, as recorded in the statement), the functions iϕX\partial_{i}\phi_{X} and jiϕX\partial_{j}\partial_{i}\phi_{X} are continuous at every point. Finally ϕX\phi_{X} itself is continuous at every point: UU is continuous on L2L^{2} by Basic Properties of Differentiability on an Open Subset of a Real Inner Product Space §continuous (it is differentiable by Claim 2 above), and (X+ca)(X+cb)L2=cabL2=ab\lVert(X+c_{a})-(X+c_{b})\rVert_{L^{2}}=\lVert c_{a-b}\rVert_{L^{2}}=\lVert a-b\rVert by The Space of Square-Integrable Random Vectors §classes and The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation §constants, so for ε>0\varepsilon>0 the δ\delta of the continuity of UU at X+cbX+c_{b} gives ϕX(a)ϕX(b)<ε|\phi_{X}(a)-\phi_{X}(b)|<\varepsilon whenever ab<δ\lVert a-b\rVert<\delta, which is continuity at bb in the sense of Continuous Map Between Metric Spaces for dEd_{E} and dRd_{\mathbb{R}}, hence in the Euclidean sense by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions. Therefore ϕX\phi_{X} is of class C1C^{1} by clause 1 of C^k Maps on a Euclidean Open Set, each iϕX\partial_{i}\phi_{X} is of class C1C^{1} by the same clause, and ϕX\phi_{X} is of class C2C^{2} by clause 2 there. So UU is twice continuously differentiable along translations at XX (The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §translations), hence on the whole space as XX was arbitrary (The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §on-space), and by The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors §laplacian, The Laplacian of a Twice Continuously Differentiable Function §laplacian and X+0Rd=XX+0_{\mathbb{R}^{d}}=X,

ΔtrU(X)=i=1diiϕX(0Rd)=i=1dE[iifX]=E[i=1diifX]=E[ΔfX],\Delta_{\mathrm{tr}}U(X)=\sum_{i=1}^{d}\partial_{i}\partial_{i}\phi_{X}(0_{\mathbb{R}^{d}})=\sum_{i=1}^{d}\mathbb{E}[\partial_{i}\partial_{i}f\circ X]=\mathbb{E}\Bigl[\sum_{i=1}^{d}\partial_{i}\partial_{i}f\circ X\Bigr]=\mathbb{E}[\Delta f\circ X],

the third equality by Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions §integrable and Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions §linear, each summand being integrable as in Step B. Lastly Δf\Delta f is Borel and bounded by dM2d\,M_{2} (claims 2 and 5 of Properties of Finite Sums and the constant sum), hence integrable with respect to L(X)\mathcal{L}(X) by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures, and E[ΔfX]=ΔfdL(X)\mathbb{E}[\Delta f\circ X]=\int\Delta f\,d\mathcal{L}(X) by Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §expectation. The class of XX being arbitrary and L(X)\mathcal{L}(X) being the same for all representatives by The Space of Square-Integrable Random Vectors §law, the identity holds for every representative.

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