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Proof of The Lifted Free Score: Norm, Weak Identity and the Second-Moment Identity

lemmalem:free-score-lift-2026a
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· 7,136 chars · 20 deps · depth 30 Reason: Batch C: proof of the lifted free score identities.

The norm and weak identities are the isometry of composition applied to the free score. For the second-moment identity, the difference quotients of the second-moment test functions are bounded by a constant not depending on the index and equal one on the ball of radius the index, so their integrals against the product measure converge to one by dominated convergence; continuity of the inner product along the convergence of the gradients to the identity, and uniqueness of limits, then give the identity, which lifts by the isometry.

Proof

Each result cited is universally quantified over the data in its own statement. The identifications of One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative are in force, in particular x=x\lVert x\rVert=|x| for xRx\in\mathbb{R} (One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative §scalars), and ι:NR\iota:\mathbb{N}\to\mathbb{R} is the canonical map of The Canonical Map from the Natural Numbers to a Field. Convergence of a sequence of real numbers is that of Limit of a Sequence of Real Numbers, read as stipulated in the preamble of Convergence and the Cauchy Condition for Real Sequences Agree with Those in the Real Line as a Metric Space: for a sequence (am)mN(a_{m})_{m\in\mathbb{N}} the indices nn for which ana_{n} is defined are exactly those of the form n=ι(m)n=\iota(m) with mNm\in\mathbb{N}, and for these the condition "nNn\ge N" reads ι(N)ι(m)\iota(N)\le\iota(m). For every νP2Φ(R)\nu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}) we have νP2(R)\nu\in\mathcal{P}_{2}(\mathbb{R}) by Finite Free Fisher Information, the Free Score and the Free Fisher Information of a Probability Measure on the Real Line §finite, and ΞνTνL2(ν;R)\Xi_{\nu}\in T_{\nu}\subseteq L^{2}(\nu;\mathbb{R}) by Finite Free Fisher Information, the Free Score and the Free Fisher Information of a Probability Measure on the Real Line §score and Basic Properties of the Tangent Space: Closed Subspace, the Identity Map Belongs to It, Second-Moment Limits, and Representation of Bounded Functionals on Gradients §closed; L2(ν;R)L^{2}(\nu;\mathbb{R}) is a real Hilbert space with distance dνd_{\nu} by Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §l2mu.

Step 1: claim 1. Suppose that the law μ=L(X)\mu=\mathcal{L}(X) lies in P2Φ(R)\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}). By Composition of a Square-Integrable Vector Field with a Random Vector, and the Lifted Score: Isometry, Norm, Weak Identity and Second-Moment Identity §composition, applied with d=1d=1, ΞμXL2=Ξμμ\lVert\Xi_{\mu}\circ X\rVert_{L^{2}}=\lVert\Xi_{\mu}\rVert_{\mu}, so ΞμXL22=Ξμμ2=Φ(μ)\lVert\Xi_{\mu}\circ X\rVert_{L^{2}}^{2}=\lVert\Xi_{\mu}\rVert_{\mu}^{2}=\Phi^{*}(\mu) by Finite Free Fisher Information, the Free Score and the Free Fisher Information of a Probability Measure on the Real Line §information. Let ψCc(R)\psi\in C_{c}^{\infty}(\mathbb{R}); then ψ=ψ\psi'=\nabla\psi by One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative §derivatives, and its class lies in L2(μ;R)L^{2}(\mu;\mathbb{R}) by Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §test, so Composition of a Square-Integrable Vector Field with a Random Vector, and the Lifted Score: Isometry, Norm, Weak Identity and Second-Moment Identity §composition gives ΞμX,ψXL2=Ξμ,ψμ\langle\Xi_{\mu}\circ X,\psi'\circ X\rangle_{L^{2}}=\langle\Xi_{\mu},\nabla\psi\rangle_{\mu}, which equals R2Fψd(μμ)\int_{\mathbb{R}^{2}}F_{\psi}\,d(\mu\boxtimes\mu) by Finite Free Fisher Information, the Free Score and the Free Fisher Information of a Probability Measure on the Real Line §score.

Step 2: the limit of the difference-quotient integrals. Let νP2Φ(R)\nu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), and for nNn\in\mathbb{N} let ψn\psi_{n} be the second-moment test function of the preamble of Basic Properties of the Tangent Space: Closed Subspace, the Identity Map Belongs to It, Second-Moment Limits, and Representation of Bounded Functionals on Gradients, applied with ν\nu in place of μ\mu and with d=1d=1: ψn\psi_{n} is the function ψR\psi_{R} of Scaled Cutoffs and the Second-Moment Test Functions: Uniform Derivative Bounds and Agreement on a Ball for the dimension q=1q=1 and R=ι(n)R=\iota(n), positive by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field, and it is a test function, as recorded there. Fix a nonnegative real number MM as in Scaled Cutoffs and the Second-Moment Test Functions: Uniform Derivative Bounds and Agreement on a Ball §test for q=1q=1, not depending on RR; since qM=ι(1)M=MqM=\iota(1)M=M by claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field, that clause gives Δψn(t)M|\Delta\psi_{n}(t)|\le M for all nNn\in\mathbb{N} and tRt\in\mathbb{R}. Hence, by One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative §quotient, each FψnF_{\psi_{n}} is Borel and Fψn(z)M|F_{\psi_{n}}(z)|\le M for all zR2z\in\mathbb{R}^{2} and nNn\in\mathbb{N}.

Pointwise limit. Fix (x,y)R2(x,y)\in\mathbb{R}^{2}. By claim 1 of The Archimedean Property of the Real Numbers there are n1,n2Nn_{1},n_{2}\in\mathbb{N} with x<ι(n1)|x|<\iota(n_{1}) and y<ι(n2)|y|<\iota(n_{2}); put n0=n1+n2n_{0}=n_{1}+n_{2}. By claim 6 of Properties of the Order on the Natural Numbers, n1<n1+n2=n0n_{1}<n_{1}+n_{2}=n_{0}, and n2<n2+n1=n0n_{2}<n_{2}+n_{1}=n_{0} by the same claim and claim 4 of Arithmetic of Addition on the Natural Numbers; so ι(n1)<ι(n0)\iota(n_{1})<\iota(n_{0}) and ι(n2)<ι(n0)\iota(n_{2})<\iota(n_{0}) by claim 6 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field, and x<ι(n0)|x|<\iota(n_{0}), y<ι(n0)|y|<\iota(n_{0}) by claim 2 of Elementary Order Arithmetic in an Ordered Field (a strict inequality implying the weak one). Now let mNm\in\mathbb{N} satisfy ι(n0)ι(m)\iota(n_{0})\le\iota(m). Then x=x<ι(m)\lVert x\rVert=|x|<\iota(m) and y<ι(m)\lVert y\rVert<\iota(m) by claim 2 of Elementary Order Arithmetic in an Ordered Field, so Scaled Cutoffs and the Second-Moment Test Functions: Uniform Derivative Bounds and Agreement on a Ball §ball, applied with the positive number R=ι(m)R=\iota(m), gives 1ψm(x)=x1=x\partial_{1}\psi_{m}(x)=x_{1}=x, 1ψm(y)=y\partial_{1}\psi_{m}(y)=y and Δψm(x)=q\Delta\psi_{m}(x)=q, read as ι(1)\iota(1) by the preamble of that lemma, which is 11 by claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field; and ψm=1ψm\psi_{m}'=\partial_{1}\psi_{m} by One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative §derivatives. If xyx\ne y, then Fψm(x,y)=(xy)(xy)1=1F_{\psi_{m}}(x,y)=(x-y)(x-y)^{-1}=1; if x=yx=y, then Fψm(x,x)=Δψm(x)=1F_{\psi_{m}}(x,x)=\Delta\psi_{m}(x)=1. Thus, for every real ε>0\varepsilon>0, Fψm(x,y)1=0<ε|F_{\psi_{m}}(x,y)-1|=0<\varepsilon for every mNm\in\mathbb{N} with ι(n0)ι(m)\iota(n_{0})\le\iota(m), that is, the real sequence (Fψn(x,y))nN(F_{\psi_{n}}(x,y))_{n\in\mathbb{N}} converges to 11.

Dominated convergence. By Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs and Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures, ννP(R2)\nu\boxtimes\nu\in\mathcal{P}(\mathbb{R}^{2}) is a Borel measure on the metric space (R2,dE)(\mathbb{R}^{2},d_{E}) with (νν)(R2)=1(\nu\boxtimes\nu)(\mathbb{R}^{2})=1, and B(R2)\mathcal{B}(\mathbb{R}^{2}) is its Borel σ\sigma-algebra (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §spaces); so by claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space the constant functions with values MM and 11 on R2\mathbb{R}^{2} are integrable with respect to νν\nu\boxtimes\nu, with R21d(νν)=1(νν)(R2)=1\int_{\mathbb{R}^{2}}1\,d(\nu\boxtimes\nu)=1\cdot(\nu\boxtimes\nu)(\mathbb{R}^{2})=1. Dominated Convergence Theorem, applied on the measure space (R2,B(R2),νν)(\mathbb{R}^{2},\mathcal{B}(\mathbb{R}^{2}),\nu\boxtimes\nu) to the sequence fn=Fψnf_{n}=F_{\psi_{n}} of Borel functions, the limit function f=1f=1 and the dominating function g=Mg=M, yields

R2Fψnd(νν)R21d(νν)=1(n).\int_{\mathbb{R}^{2}}F_{\psi_{n}}\,d(\nu\boxtimes\nu)\to\int_{\mathbb{R}^{2}}1\,d(\nu\boxtimes\nu)=1\qquad(n\to\infty).

Step 3: claim 2. Let ν\nu and ψn\psi_{n} be as in Step 2. By Finite Free Fisher Information, the Free Score and the Free Fisher Information of a Probability Measure on the Real Line §score applied to ψn\psi_{n}, the real sequence an=Ξν,ψnν=R2Fψnd(νν)a_{n}=\langle\Xi_{\nu},\nabla\psi_{n}\rangle_{\nu}=\int_{\mathbb{R}^{2}}F_{\psi_{n}}\,d(\nu\boxtimes\nu) converges to 11 by Step 2. By the symmetry of the inner product (Real Inner Product Space §inner-product), an=ψn,Ξννa_{n}=\langle\nabla\psi_{n},\Xi_{\nu}\rangle_{\nu}. Since ψnid\nabla\psi_{n}\to\mathrm{id} in the metric space (L2(ν;R),dν)(L^{2}(\nu;\mathbb{R}),d_{\nu}) by Basic Properties of the Tangent Space: Closed Subspace, the Identity Map Belongs to It, Second-Moment Limits, and Representation of Bounded Functionals on Gradients §identity, the last assertion of The Norm Metric of a Real Inner Product Space: Triangle Inequalities, Limits and Continuity §continuity, applied in the real inner product space L2(ν;R)L^{2}(\nu;\mathbb{R}) with z=Ξνz=\Xi_{\nu}, shows that (an)(a_{n}) converges to id,Ξνν=Ξν,idν\langle\mathrm{id},\Xi_{\nu}\rangle_{\nu}=\langle\Xi_{\nu},\mathrm{id}\rangle_{\nu}. By claim 1 of Uniqueness of Limits and Boundedness of Convergent Real Sequences, Ξν,idν=1\langle\Xi_{\nu},\mathrm{id}\rangle_{\nu}=1. If μP2Φ(R)\mu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), this applies to ν=μ\nu=\mu, and by Composition of a Square-Integrable Vector Field with a Random Vector, and the Lifted Score: Isometry, Norm, Weak Identity and Second-Moment Identity §composition, ΞμX,XL2=ΞμX,idXL2=Ξμ,idμ=1\langle\Xi_{\mu}\circ X,X\rangle_{L^{2}}=\langle\Xi_{\mu}\circ X,\mathrm{id}\circ X\rangle_{L^{2}}=\langle\Xi_{\mu},\mathrm{id}\rangle_{\mu}=1.

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