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Proof of The Constant Tuple on L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}): Coordinates, Projection, Tail Form, and Translation-Closed Preimages

lemmalem:constants-tuple-lift-wasserstein-2026a
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· 9,360 chars · 22 deps · depth 34 Reason: First publication: identifies the coordinate map, projection and tail form of the constant tuple and proves translation closure of preimages under the law map.

The inner product against a constant class is the corresponding coordinate of the mean of the law; orthonormality and the identification of the projection and tail form follow, and translation closure follows from the law of a shifted class.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied here to the data named in the statement of the lemma. Throughout, XL2(Ω;Rd)X\in L^{2}(\Omega;\mathbb{R}^{d}), aRda\in\mathbb{R}^{d} and i,j[d]i,j\in[d] are arbitrary, a class and a representative of it are written alike as Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §dimensions prescribes, and E\mathbb{E} is the expectation with respect to PP. The space L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}) is a real Hilbert space by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §hilbert and 1d1\le d, so once γ\gamma is known to be orthonormal, which is Step 3, Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions applies to it as the statement describes.

Step 1 (the inner product against a constant class). By the definition of the inner product, X,ceiL2=E[Xcei]\langle X,c_{e_{i}}\rangle_{L^{2}}=\mathbb{E}[X\cdot c_{e_{i}}], where XceiX\cdot c_{e_{i}} is the random variable of Basic Properties of Random Vectors: Coordinates, Borel Images and Arithmetic, Change of Variables, Almost Sure Equality and Pairs §composition; a representative of ceic_{e_{i}} is the constant map with value eie_{i} by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §constants, so the value of that random variable at ωΩ\omega\in\Omega is X(ω)eiX(\omega)\cdot e_{i}. By Real Matrices, Symmetric Matrices and the Semidefinite Ordering: Standing Notation §basis the iith coordinate of a point zRdz\in\mathbb{R}^{d} equals zeiz\cdot e_{i}, so X(ω)eiX(\omega)\cdot e_{i} is the value at ω\omega of the coordinate XiX_{i}; that is, Xcei=XiX\cdot c_{e_{i}}=X_{i}. The law L(X)\mathcal{L}(X) belongs to P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §law, so The Mean of a Square-Integrable Probability Measure, Its Lift, Its Centring, and Functions of the Mean and Centred Integrals as Test Functions §mean applies to it and gives that XiX_{i} is integrable with E[Xi]=m(L(X))i\mathbb{E}[X_{i}]=m(\mathcal{L}(X))_{i}. Hence

X,ceiL2=m(L(X))i,\langle X,c_{e_{i}}\rangle_{L^{2}}=m\bigl(\mathcal{L}(X)\bigr)_{i},

which is the first identity of clause 3.

Step 2 (clause 1). A representative of cac_{a} is the constant map with value aa (The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §constants), so its coordinate (ca)i(c_{a})_{i} is the constant map ΩR\Omega\to\mathbb{R} with value aia_{i}, which is the map ai1Ωa_{i}\mathbf{1}_{\Omega} for the indicator function 1Ω\mathbf{1}_{\Omega} of the set Ω\Omega, an element of F\mathcal{F} because F\mathcal{F} is a σ\sigma-algebra on Ω\Omega. By The Integral of an Indicator Function is the Measure of the Set the function 1Ω\mathbf{1}_{\Omega} is a nonnegative simple function with Ω1ΩdP=P(Ω)\int_{\Omega}\mathbf{1}_{\Omega}\,dP=P(\Omega), and P(Ω)=1P(\Omega)=1 because PP is a probability measure (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §probability-space); being nonnegative, 1Ω\mathbf{1}_{\Omega} equals its own absolute value, so Ω1ΩdP=1\int_{\Omega}|\mathbf{1}_{\Omega}|\,dP=1 and 1Ω\mathbf{1}_{\Omega} is integrable. Claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with 1Ω\mathbf{1}_{\Omega} in both function slots and with the scalars aia_{i} and 00, gives that ai1Ωa_{i}\mathbf{1}_{\Omega} is integrable with

Ωai1ΩdP=aiΩ1ΩdP+0Ω1ΩdP=ai.\int_{\Omega}a_{i}\mathbf{1}_{\Omega}\,dP=a_{i}\int_{\Omega}\mathbf{1}_{\Omega}\,dP+0\int_{\Omega}\mathbf{1}_{\Omega}\,dP=a_{i}.

Thus E[(ca)i]=ai\mathbb{E}[(c_{a})_{i}]=a_{i} by Expectation, Variance, and Moments, and m(L(ca))i=aim(\mathcal{L}(c_{a}))_{i}=a_{i} by The Mean of a Square-Integrable Probability Measure, Its Lift, Its Centring, and Functions of the Mean and Centred Integrals as Test Functions §mean applied to cac_{a}. As ii was arbitrary and points of Rd\mathbb{R}^{d} with the same coordinates coincide (Euclidean Points as Tuples of Real Numbers), m(L(ca))=am(\mathcal{L}(c_{a}))=a. Finally M2(L(ca))=caL22=a2M_{2}(\mathcal{L}(c_{a}))=\lVert c_{a}\rVert_{L^{2}}^{2}=\lVert a\rVert^{2} by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §law and The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §constants. This proves clause 1.

Step 3 (clause 2). By The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §constants and Real Matrices, Symmetric Matrices and the Semidefinite Ordering: Standing Notation §basis, ceiL2=ei=1\lVert c_{e_{i}}\rVert_{L^{2}}=\lVert e_{i}\rVert=1 for every ii. Let iji\ne j. Step 1, applied to the class ceic_{e_{i}} and the index jj, gives cei,cejL2=m(L(cei))j\langle c_{e_{i}},c_{e_{j}}\rangle_{L^{2}}=m(\mathcal{L}(c_{e_{i}}))_{j}, which equals (ei)j(e_{i})_{j} by clause 1; and (ei)j=0(e_{i})_{j}=0, because eie_{i} is the point whose iith coordinate is 11 and whose other coordinates are 00 (Real Matrices, Symmetric Matrices and the Semidefinite Ordering: Standing Notation §basis) and jij\ne i. Both conditions of Orthogonality, Orthogonal Complement and Orthonormal Families in a Real Inner Product Space §orthonormal therefore hold for γ\gamma, which is clause 2.

Step 4 (the coordinate map). By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §coordinates the coordinate map determined by γ\gamma sends XX to the point of Rd\mathbb{R}^{d} whose iith coordinate is X,ceiL2\langle X,c_{e_{i}}\rangle_{L^{2}} for each i[d]i\in[d]. By Step 1 that coordinate is m(L(X))im(\mathcal{L}(X))_{i}, so the point is m(L(X))m(\mathcal{L}(X)) by Euclidean Points as Tuples of Real Numbers. Since m(L(X))m(\mathcal{L}(X)) is determined by L(X)\mathcal{L}(X), the map takes equal values at two classes with the same law.

Step 5 (the tail form as a centred second moment). Let ZL2(Ω;Rd)Z\in L^{2}(\Omega;\mathbb{R}^{d}). By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail one has ZL22=Π(Z,Z)+N(Z,Z)\lVert Z\rVert_{L^{2}}^{2}=\Pi(Z,Z)+N(Z,Z), where Π\Pi is the projection form of γ\gamma and Π(Z,Z)\Pi(Z,Z) is the squared Euclidean norm of the image of ZZ under the coordinate map, hence m(L(Z))2\lVert m(\mathcal{L}(Z))\rVert^{2} by Step 4; and ZL22=M2(L(Z))\lVert Z\rVert_{L^{2}}^{2}=M_{2}(\mathcal{L}(Z)) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §law. Therefore

N(Z,Z)=M2(L(Z))m(L(Z))2.N(Z,Z)=M_{2}\bigl(\mathcal{L}(Z)\bigr)-\bigl\lVert m(\mathcal{L}(Z))\bigr\rVert^{2}.

Step 6 (the identity Λa=ca\Lambda^{\sharp}a=c_{a}). Apply Step 5 to cac_{a}: by clause 1 both M2(L(ca))M_{2}(\mathcal{L}(c_{a})) and m(L(ca))2\lVert m(\mathcal{L}(c_{a}))\rVert^{2} equal a2\lVert a\rVert^{2}, so N(ca,ca)=0N(c_{a},c_{a})=0. By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail also N(ca,ca)=caJcaL22N(c_{a},c_{a})=\lVert c_{a}-Jc_{a}\rVert_{L^{2}}^{2}, so the nonnegative real number caJcaL2\lVert c_{a}-Jc_{a}\rVert_{L^{2}} has square 0=000=0\cdot0 and is therefore 00 by claim 3 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field; hence caJcac_{a}-Jc_{a} is the zero vector by Elementary Identities in a Real Inner Product Space §vanishing, and ca=Jcac_{a}=Jc_{a}, L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}) being a real vector space. On the other hand JJ is the coordinate map followed by Λ\Lambda^{\sharp} (Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §coordinates), so Jca=Λ(m(L(ca)))=ΛaJc_{a}=\Lambda^{\sharp}\bigl(m(\mathcal{L}(c_{a}))\bigr)=\Lambda^{\sharp}a by Step 4 and clause 1. Therefore Λa=ca\Lambda^{\sharp}a=c_{a}.

Step 7 (the remaining assertions of clauses 3 and 4). By Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §coordinates the dot product of aa with the image of XX under the coordinate map equals Λa,XL2\langle\Lambda^{\sharp}a,X\rangle_{L^{2}}; by Steps 4 and 6 this reads am(L(X))=ca,XL2a\cdot m(\mathcal{L}(X))=\langle c_{a},X\rangle_{L^{2}}, the second identity of clause 3. Together with Steps 4 and 6 this proves clause 3.

For clause 4, JX=Λ(m(L(X)))=cm(L(X))JX=\Lambda^{\sharp}\bigl(m(\mathcal{L}(X))\bigr)=c_{m(\mathcal{L}(X))} by the description of JJ in Step 6 and by Steps 4 and 6. Hence, by Coordinate Maps of a Finite Orthonormal Tuple: Forms, the Tail Form, and Quadratic Test Functions §tail,

N(X,X)=XJXL22=Xcm(L(X))L22.N(X,X)=\lVert X-JX\rVert_{L^{2}}^{2}=\bigl\lVert X-c_{m(\mathcal{L}(X))}\bigr\rVert_{L^{2}}^{2}.

The law of Xcm(L(X))X-c_{m(\mathcal{L}(X))} is L(X)\overline{\mathcal{L}(X)} by The Mean of a Square-Integrable Probability Measure, Its Lift, Its Centring, and Functions of the Mean and Centred Integrals as Test Functions §centring, so the right-hand side equals M2(L(X))M_{2}(\overline{\mathcal{L}(X)}) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §law; and it equals M2(L(X))m(L(X))2M_{2}(\mathcal{L}(X))-\lVert m(\mathcal{L}(X))\rVert^{2} by Step 5. Each of these expressions is determined by L(X)\mathcal{L}(X), so N(X,X)N(X,X) takes equal values at two classes with the same law. This proves clause 4.

Step 8 (clause 5). Assume that (Ω,F,P)(\Omega,\mathcal{F},P) is rich and let QQ be as in clause 5. Since QQ is nonempty there is μQ\mu\in Q, and by The Wasserstein Distance and the Mean-Square Distance of Random Vectors §onto there is XL2(Ω;Rd)X\in L^{2}(\Omega;\mathbb{R}^{d}) with L(X)=μ\mathcal{L}(X)=\mu; then XQΛX\in Q^{\Lambda}, so QΛQ^{\Lambda} is nonempty. Let XQΛX\in Q^{\Lambda} and aRda\in\mathbb{R}^{d}. By Step 6, X+Λa=X+caX+\Lambda^{\sharp}a=X+c_{a}, and L(X+ca)=(τa)#L(X)\mathcal{L}(X+c_{a})=(\tau_{a})_{\#}\mathcal{L}(X) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations §constants, which lies in QQ by the hypothesis on QQ, since L(X)Q\mathcal{L}(X)\in Q. Hence X+ΛaQΛX+\Lambda^{\sharp}a\in Q^{\Lambda}, and QΛQ^{\Lambda} is translation-closed along γ\gamma by Subsets of a Real Hilbert Space Translation-Closed along an Orthonormal Tuple §closed.

Step 9 (clause 6). The penalty domain D\mathcal{D} contains the score domain DΣ\mathcal{D}_{\Sigma} by Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §pair, and DΣ\mathcal{D}_{\Sigma} is nonempty by Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §nonempty, so D\mathcal{D} is nonempty; and (τa)#μD(\tau_{a})_{\#}\mu\in\mathcal{D} for every μD\mu\in\mathcal{D} and every aRda\in\mathbb{R}^{d} by Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §translation-invariant. Clause 5, applied with D\mathcal{D} in the role of QQ, gives that DΛ\mathcal{D}^{\Lambda} is translation-closed along γ\gamma. This proves clause 6 and completes the proof of the lemma.

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