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Proof of Splitting a Bounded First Variation into a Square-Integrable Potential Force and a Finite Fisher Information

lemmalem:confining-score-splitting-euclidean-2026a
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· 6,901 chars · 22 deps · depth 29 Reason: E2 Stage 1: proof of the splitting lemma.

Test the hypothesis, extended by approximation from test functions, on the concave truncations kU/(k+U) of the shifted potential U. Concavity lets the curvature term be dropped, giving a quadratic inequality that bounds the truncated force uniformly in k; monotone convergence then gives square-integrability of the force, and the hypothesis bounds the Laplacian term.

Proof

Each result cited is universally quantified over the data in its own statement. Write (ψ)=VψdμκΔψdμ\ell(\psi)=\int\nabla V\cdot\nabla\psi\,d\mu-\kappa\int\Delta\psi\,d\mu.

Claim 1. By Basic Properties of a Confining Potential on Euclidean Space: Continuity, Quadratic Minorants, the Tangent Inequality, Hessian Bounds, Growth under Translation, and Integrability §integrable, μP2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}) and V\lVert\nabla V\rVert and ΔV\Delta V are μ\mu-integrable. Let ψCc(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}). The maps V\nabla V (Basic Properties of a Confining Potential on Euclidean Space: Continuity, Quadratic Minorants, the Tangent Inequality, Hessian Bounds, Growth under Translation, and Integrability §regularity) and ψ\nabla\psi (claim 1 of The Gradient of a Test Function is Bounded and Square-Integrable, and Its Laplacian Bounded and Integrable, Against Every Probability Measure) are Borel, so Vψ\nabla V\cdot\nabla\psi is Borel by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §functions. With KK the bound on ψ\lVert\nabla\psi\rVert from that claim, VψKV|\nabla V\cdot\nabla\psi|\le K\lVert\nabla V\rVert by Cauchy-Schwarz Inequality for the Euclidean Dot Product, so Vψ\nabla V\cdot\nabla\psi is integrable: a Borel function whose absolute value is dominated by an integrable function has finite integral of its absolute value, by monotonicity of the integral (claim 1 of Linearity and Monotonicity of the Lebesgue Integral), hence is integrable. The same remark is used below whenever integrability follows from such a bound.

Constants. Let v0v_{0} be as in Basic Properties of a Confining Potential on Euclidean Space: Continuity, Quadratic Minorants, the Tangent Inequality, Hessian Bounds, Growth under Translation, and Integrability §growth, so v0Vv_{0}\le V, and let U=Vv0+1U=V-v_{0}+1, a C2C^{2} function with 1U1\le U and the same partial derivatives as VV. Let C1C_{1} be the constant of Confining Potentials on Euclidean Space §slope, let CC' be the constant of Confining Potentials on Euclidean Space §curvature for ε=1\varepsilon=1, and let c0=v0+1c_{0}=|v_{0}|+1. Then VU+c0(1+c0)U|V|\le U+c_{0}\le(1+c_{0})U, so, with A=C1(2+c0)A=|C_{1}|(2+c_{0}) and B=2+c0+CB=2+c_{0}+|C'|,

VC1(1+V)AU,jiVΔVV+CBU,\lVert\nabla V\rVert\le|C_{1}|(1+|V|)\le A\,U,\qquad|\partial_{j}\partial_{i}V|\le\Delta V\le|V|+C'\le B\,U,

the middle bound by Basic Properties of a Confining Potential on Euclidean Space: Continuity, Quadratic Minorants, the Tangent Inequality, Hessian Bounds, Growth under Translation, and Integrability §hessian; again 1U1\le U is used.

Step 1 (the truncations). For pNp\in\mathbb{N}, read as a positive real number, let Gp:(p,)RG_{p}:(-p,\infty)\to\mathbb{R} be Gp(u)=pp2(p+u)1=pu(p+u)1G_{p}(u)=p-p^{2}(p+u)^{-1}=pu(p+u)^{-1}. By Reciprocal Rule for One-Dimensional Derivatives and Chain Rule for One-Dimensional Derivatives, GpG_{p} is twice differentiable on the open interval (p,)(-p,\infty), with

Gp(u)=p2(p+u)2,Gp(u)=2p2(p+u)3,G_{p}'(u)=p^{2}(p+u)^{-2},\qquad G_{p}''(u)=-2p^{2}(p+u)^{-3},

both continuous; so GpG_{p} is of class C2C^{2} on (p,)R1(-p,\infty)\subseteq\mathbb{R}^{1}, its partial derivative being its derivative (Partial Derivative on a Euclidean Open Set). Since UU takes values in [1,)(p,)[1,\infty)\subseteq(-p,\infty), the function fp=GpUf_{p}=G_{p}\circ U is of class C2C^{2} on Rd\mathbb{R}^{d} by claim 2 of A Composition of CkC^k Maps Between Euclidean Open Sets is of Class CkC^k, and by its claim 1 and the product rule

ifp=wpiV,jifp=wpjiV+Gp(U)iVjV,wp=Gp(U)=(1+p1U)2.\partial_{i}f_{p}=w_{p}\,\partial_{i}V,\qquad\partial_{j}\partial_{i}f_{p}=w_{p}\,\partial_{j}\partial_{i}V+G_{p}''(U)\,\partial_{i}V\,\partial_{j}V,\qquad w_{p}=G_{p}'(U)=\bigl(1+p^{-1}U\bigr)^{-2}.

Since U1>0U\ge1>0, one has 0<wp10<w_{p}\le1, Gp(U)<0G_{p}''(U)<0, p(p+U)11p(p+U)^{-1}\le1 and U(p+U)11U(p+U)^{-1}\le1. Hence ifpp2(p+U)2AUAp|\partial_{i}f_{p}|\le p^{2}(p+U)^{-2}AU\le Ap and

jifpp2(p+U)2BU+2p2(p+U)3A2U2Bp+2A2p.|\partial_{j}\partial_{i}f_{p}|\le p^{2}(p+U)^{-2}BU+2p^{2}(p+U)^{-3}A^{2}U^{2}\le Bp+2A^{2}p .

So the first and second partial derivatives of fpf_{p} are bounded by Mp=(A+B+2A2)pM_{p}=(A+B+2A^{2})p.

Step 2 (the hypothesis for fpf_{p}). By Approximation of a Twice Continuously Differentiable Function with Bounded First and Second Derivatives by Test Functions §approximation (with q=dq=d, f=fpf=f_{p}, M=MpM=M_{p}) there are test functions ψn\psi_{n} and M0M'\ge0 whose first and second partial derivatives are bounded by MM' and converge pointwise to those of fpf_{p}. Then pointwise VψnVfp\nabla V\cdot\nabla\psi_{n}\to\nabla V\cdot\nabla f_{p}, with VψndMV|\nabla V\cdot\nabla\psi_{n}|\le\sqrt{d}M'\lVert\nabla V\rVert; ΔψnΔfp\Delta\psi_{n}\to\Delta f_{p}, with ΔψndM|\Delta\psi_{n}|\le dM'; and ψn2fp2\lVert\nabla\psi_{n}\rVert^{2}\to\lVert\nabla f_{p}\rVert^{2}, with ψn2dM2\lVert\nabla\psi_{n}\rVert^{2}\le dM'^{2}; the limits are by Arithmetic of Limits of Real Sequences. The dominating functions are integrable (Claim 1, and μ\mu is a probability measure), so Dominated Convergence Theorem and continuity of the square root pass the hypothesis (ψn)Cψnμ|\ell(\psi_{n})|\le C\lVert\nabla\psi_{n}\rVert_{\mu} to the limit:

VfpdμκΔfpdμCXp,Xp=(wp2V2dμ)1/2.(1)\Bigl|\int\nabla V\cdot\nabla f_{p}\,d\mu-\kappa\int\Delta f_{p}\,d\mu\Bigr|\le C\,X_{p},\qquad X_{p}=\Bigl(\int w_{p}^{2}\lVert\nabla V\rVert^{2}\,d\mu\Bigr)^{1/2}.\tag{1}

Step 3 (dropping the curvature term). By Step 1, Vfp=wpV2\nabla V\cdot\nabla f_{p}=w_{p}\lVert\nabla V\rVert^{2} and Δfp=wpΔV+Gp(U)V2\Delta f_{p}=w_{p}\Delta V+G_{p}''(U)\lVert\nabla V\rVert^{2}. All of these functions are integrable: wpV2w_{p}\lVert\nabla V\rVert^{2} by Claim 1 applied through Step 2, 0wpΔVΔV0\le w_{p}\Delta V\le\Delta V, and Gp(U)V2=ΔfpwpΔVG_{p}''(U)\lVert\nabla V\rVert^{2}=\Delta f_{p}-w_{p}\Delta V. Since κ>0\kappa>0, Gp(U)0G_{p}''(U)\le0, 0ΔV0\le\Delta V and wp2wp1w_{p}^{2}\le w_{p}\le1,

VfpdμκΔfpdμwpV2dμκΔVdμXp2D,D=κΔVdμ0.\int\nabla V\cdot\nabla f_{p}\,d\mu-\kappa\int\Delta f_{p}\,d\mu\ge\int w_{p}\lVert\nabla V\rVert^{2}\,d\mu-\kappa\int\Delta V\,d\mu\ge X_{p}^{2}-D,\qquad D=\kappa\int\Delta V\,d\mu\ge0 .

With (1), Xp2CXp+DX_{p}^{2}\le CX_{p}+D. Hence XpC+DX_{p}\le C+\sqrt{D}: otherwise Xp>C+DDX_{p}>C+\sqrt{D}\ge\sqrt{D} would give Xp2>(C+D)XpCXp+DX_{p}^{2}>(C+\sqrt{D})X_{p}\ge CX_{p}+D.

Step 4 (monotone limit). Fix xx. If ppp\le p', then 0<p1U(x)p1U(x)0<p'^{-1}U(x)\le p^{-1}U(x), so 11+p1U(x)1+p1U(x)1\le1+p'^{-1}U(x)\le1+p^{-1}U(x). Squares are monotone on nonnegative numbers (Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field), and inverses reverse the order of positive numbers (aba\le b gives b1=aa1b1ba1b1=a1b^{-1}=a\,a^{-1}b^{-1}\le b\,a^{-1}b^{-1}=a^{-1} by claim 5 of Elementary Arithmetic in an Ordered Field). Hence wp(x)wp(x)w_{p}(x)\le w_{p'}(x). Moreover p10p^{-1}\to0 (The Archimedean Property of the Real Numbers and Limit of a Sequence of Real Numbers), so wp(x)=(1+p1U(x))21w_{p}(x)=(1+p^{-1}U(x))^{-2}\to1 by Arithmetic of Limits of Real Sequences. So wp2V2w_{p}^{2}\lVert\nabla V\rVert^{2} increases pointwise to V2\lVert\nabla V\rVert^{2}, and Monotone Convergence Theorem gives V2dμ=limpXp2(C+D)2<\int\lVert\nabla V\rVert^{2}\,d\mu=\lim_{p}X_{p}^{2}\le(C+\sqrt{D})^{2}<\infty (Order Properties of Limits of Real Sequences).

Step 5 (finite Fisher information). Let ψCc(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}). By the hypothesis, and the Cauchy–Schwarz inequality in the real Hilbert space L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) (The Cauchy-Schwarz Inequality in a Real Inner Product Space),

κΔψdμ(ψ)+V,ψμ(C+Vμ)ψμ.\kappa\Bigl|\int\Delta\psi\,d\mu\Bigr|\le|\ell(\psi)|+\bigl|\langle\nabla V,\nabla\psi\rangle_{\mu}\bigr|\le\bigl(C+\lVert\nabla V\rVert_{\mu}\bigr)\lVert\nabla\psi\rVert_{\mu}.

Dividing by κ>0\kappa>0 gives the inequality of Finite Fisher Information, the Score and the Fisher Information of a Probability Measure §finite with constant κ1(C+Vμ)\kappa^{-1}(C+\lVert\nabla V\rVert_{\mu}). Since μP2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}) by Claim 1, μP2I(Rd)\mu\in\mathcal{P}_{2}^{\mathcal{I}}(\mathbb{R}^{d}). \blacksquare

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