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Proof of The Entropy of the Push-Forward of a Measure by the Gradient of a Twice Continuously Differentiable Function with Pinched Hessian

lemmalem:entropy-pushforward-gradient-map-2026a
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The gradient map is a bijection with symmetric positive definite Jacobian matrix equal to the Hessian and continuously differentiable inverse, so the change-of-variables theorem gives the density of the push-forward; the pointwise identity for s log s at that density, integrated with the change-of-variables formula, yields the entropy formula, while the Lipschitz bound controls the second moment.

Proof

Each result cited below is universally quantified over the data in its own statement. Write F=ΦF=\nabla\Phi, j(x)=detD2Φ(x)j(x)=\det D^{2}\Phi(x) and (x)=logj(x)\ell(x)=\log j(x) for xRdx\in\mathbb{R}^{d}, let λd\lambda_{d} be Lebesgue measure, let densities with respect to λd\lambda_{d} be those of The Radon-Nikodym Theorem for a Finite Measure and a Sigma-Finite Measure, and Uniqueness of Densities, and let ϕ\phi be the function sslogss\mapsto s\log s of The Function slogss\log s: Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm.

Claim 1 (The map FF). FF satisfies the hypotheses of Change of Variables for the Lebesgue Integral under a Continuously Differentiable Bijection of Euclidean Space with Symmetric Positive Definite Jacobian Matrix, and the Density of a Push-Forward, with DF(x)=D2Φ(x)DF(x)=D^{2}\Phi(x) and detDF(x)=j(x)>0\det DF(x)=j(x)>0 for every xx; FF and F1F^{-1} are Borel, and jj is continuous and Borel.

By The Gradient of a Twice Continuously Differentiable Function with Hessian Pinched between Two Positive Multiples of the Identity is a Bi-Lipschitz Bijection of Euclidean Space with Continuously Differentiable Inverse §bijection, FF is a bijection of Rd\mathbb{R}^{d} onto Rd\mathbb{R}^{d}; write F1F^{-1} for its inverse. Since Φ\Phi is of class C2C^{2}, its partial derivatives iΦ\partial_{i}\Phi, the components of FF, are of class C1C^{1} by clause 2 of C^k Maps on a Euclidean Open Set. By The Gradient of a Twice Continuously Differentiable Function with Hessian Pinched between Two Positive Multiples of the Identity is a Bi-Lipschitz Bijection of Euclidean Space with Continuously Differentiable Inverse §inverse, for every xx the matrix D2Φ(x)D^{2}\Phi(x) is positive definite and DF(x)=D2Φ(x)DF(x)=D^{2}\Phi(x), the components of F1F^{-1} are of class C1C^{1}, and DF1(F(x))DF^{-1}(F(x)) is the inverse matrix of D2Φ(x)=DF(x)D^{2}\Phi(x)=DF(x). As D2Φ(x)S(d)D^{2}\Phi(x)\in\mathcal{S}(d) (Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives), DF(x)DF(x) is symmetric and positive definite. Hence FF satisfies the hypotheses of Change of Variables for the Lebesgue Integral under a Continuously Differentiable Bijection of Euclidean Space with Symmetric Positive Definite Jacobian Matrix, and the Density of a Push-Forward, detDF(x)=detD2Φ(x)=j(x)\det DF(x)=\det D^{2}\Phi(x)=j(x), and 0<j(x)0<j(x) by Determinants of Positive Definite Matrices: Positivity, the Bound logdetAtrAd\log\det A\le\mathrm{tr}\,A-d, Bounds under Pinching, and the Expansion of det(I+tB)\det(I+tB) §positive. The remaining assertions are Change of Variables for the Lebesgue Integral under a Continuously Differentiable Bijection of Euclidean Space with Symmetric Positive Definite Jacobian Matrix, and the Density of a Push-Forward §regularity.

Claim 2 (Second moment; claim 1). By The Gradient of a Twice Continuously Differentiable Function with Hessian Pinched between Two Positive Multiples of the Identity is a Bi-Lipschitz Bijection of Euclidean Space with Continuously Differentiable Inverse §bilipschitz, F(x)F(0Rd)dLx\lVert F(x)-F(0_{\mathbb{R}^{d}})\rVert\le d\,L\,\lVert x\rVert for every xx, so F(x)F(0Rd)2d2L2x2\lVert F(x)-F(0_{\mathbb{R}^{d}})\rVert^{2}\le d^{2}L^{2}\lVert x\rVert^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, and the second inequality of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §functions gives

F(x)22F(0Rd)2+2F(x)F(0Rd)22F(0Rd)2+2d2L2x2.\lVert F(x)\rVert^{2}\le2\lVert F(0_{\mathbb{R}^{d}})\rVert^{2}+2\lVert F(x)-F(0_{\mathbb{R}^{d}})\rVert^{2}\le2\lVert F(0_{\mathbb{R}^{d}})\rVert^{2}+2d^{2}L^{2}\lVert x\rVert^{2}.

Since FF is Borel (Claim 1), F#μP(Rd)F_{\#}\mu\in\mathcal{P}(\mathbb{R}^{d}) and, by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pushforward applied to the nonnegative Borel function yy2y\mapsto\lVert y\rVert^{2} (Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §functions) and by claim 1 of Linearity and Monotonicity of the Lebesgue Integral,

M2(F#μ)=RdF(x)2μ(dx)2F(0Rd)2+2d2L2M2(μ)<,M_{2}(F_{\#}\mu)=\int_{\mathbb{R}^{d}}\lVert F(x)\rVert^{2}\,\mu(dx)\le2\lVert F(0_{\mathbb{R}^{d}})\rVert^{2}+2d^{2}L^{2}M_{2}(\mu)<\infty,

because μ(Rd)=1\mu(\mathbb{R}^{d})=1 and μP2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}) (The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §moment, The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §space). Hence F#μP2(Rd)F_{\#}\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}).

Claim 3 (The function \ell). \ell is Borel and bounded.

For each xx the matrix D2Φ(x)D^{2}\Phi(x) lies in S(d)\mathcal{S}(d) (Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives) and satisfies εIdD2Φ(x)LId\varepsilon I_{d}\preceq D^{2}\Phi(x)\preceq L\,I_{d}, so Determinants of Positive Definite Matrices: Positivity, the Bound logdetAtrAd\log\det A\le\mathrm{tr}\,A-d, Bounds under Pinching, and the Expansion of det(I+tB)\det(I+tB) §pinching gives ddε1(x)dLdd-d\,\varepsilon^{-1}\le\ell(x)\le d\,L-d. With B=ddε1+dLdB=|d-d\,\varepsilon^{-1}|+|d\,L-d|, claims 1, 2 and 3 of Properties of the Absolute Value in an Ordered Field give (x)B\ell(x)\le B and (x)B-\ell(x)\le B, hence (x)B|\ell(x)|\le B by claim 6 there; so \ell is bounded. The logarithm is smooth on the open set (0,)(0,\infty) by The Natural Logarithm, hence continuous relative to (0,)(0,\infty) by claim 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous, hence sequentially continuous on (0,)(0,\infty) by Continuity Between Metric Spaces is Equivalent to Sequential Continuity §sequential, the Euclidean distance of R1\mathbb{R}^{1} being the absolute-value metric by Euclidean, Metric and Sequential Continuity of a Real Function of a Real Variable §distance. Since jj is Borel with values in (0,)(0,\infty) (Claim 1), =logj\ell=\log\circ j is Borel by Sequentially Continuous Functions of Measurable Euclidean Maps are Measurable.

Claim 4 (A pointwise identity). Let ρ\rho be a density of μ\mu with respect to λd\lambda_{d} and let ρ~(y)=ρ(F1(y))/j(F1(y))\tilde{\rho}(y)=\rho(F^{-1}(y))/j(F^{-1}(y)). Then ρ~\tilde{\rho} is a density of F#μF_{\#}\mu with respect to λd\lambda_{d}, and for every xRdx\in\mathbb{R}^{d}

ϕ(ρ~(F(x)))j(x)=ϕ(ρ(x))ρ(x)(x).\phi\bigl(\tilde{\rho}(F(x))\bigr)\,j(x)=\phi(\rho(x))-\rho(x)\,\ell(x).

The first assertion is Change of Variables for the Lebesgue Integral under a Continuously Differentiable Bijection of Euclidean Space with Symmetric Positive Definite Jacobian Matrix, and the Density of a Push-Forward §densities, applicable by Claim 1, which also gives detDF=j\det DF=j; in particular ρ~\tilde{\rho} is Borel and nonnegative. Since F1(F(x))=xF^{-1}(F(x))=x, ρ~(F(x))=ρ(x)j(x)1\tilde{\rho}(F(x))=\rho(x)\,j(x)^{-1}. If ρ(x)=0\rho(x)=0, both sides vanish, as ϕ(0)=0\phi(0)=0. If 0<ρ(x)0<\rho(x), then by the product rule of The Natural Logarithm (with log(j(x)1)=logj(x)\log(j(x)^{-1})=-\log j(x), since log1=logexp(0)=0\log1=\log\exp(0)=0), logρ~(F(x))=logρ(x)(x)\log\tilde{\rho}(F(x))=\log\rho(x)-\ell(x), and multiplying by ρ~(F(x))j(x)=ρ(x)\tilde{\rho}(F(x))\,j(x)=\rho(x) gives the identity.

Claim 5 (Entropy; claim 2). By Claim 3, \ell is Borel and bounded. Let ρ\rho be a density of μ\mu with respect to λd\lambda_{d} with ϕρ\phi\circ\rho integrable with respect to λd\lambda_{d} (The Entropy of a Probability Measure on Euclidean Space §entropy). The bounded Borel function \ell is integrable with respect to μ\mu by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures; since μ(A)=1Aρdλd\mu(A)=\int\mathbf{1}_{A}\rho\,d\lambda_{d} for every Borel AA, μ\mu is the measure with density ρ\rho with respect to λd\lambda_{d} of claim 3 of Image Measures, Measures with Densities, and Change of Variables, and that claim shows that ρ\rho\,\ell is integrable with respect to λd\lambda_{d} with ρdλd=dμ\int\rho\,\ell\,d\lambda_{d}=\int\ell\,d\mu. By Claim 4 and claim 2 of Linearity and Monotonicity of the Lebesgue Integral, the function (ϕρ~F)j=ϕρρ(\phi\circ\tilde{\rho}\circ F)\,j=\phi\circ\rho-\rho\,\ell is integrable with respect to λd\lambda_{d}, with integral Ent(μ)dμ\mathrm{Ent}(\mu)-\int\ell\,d\mu. The function ϕρ~\phi\circ\tilde{\rho} is Borel by The Function slogss\log s: Continuity, Young's Inequality and Lower Bounds, with the Elementary Bounds for the Exponential and the Logarithm §continuous, so by Change of Variables for the Lebesgue Integral under a Continuously Differentiable Bijection of Euclidean Space with Symmetric Positive Definite Jacobian Matrix, and the Density of a Push-Forward §integrals it is integrable with respect to λd\lambda_{d} and

Rdϕρ~dλd=Rd(ϕρ~F)detDFdλd=Ent(μ)RdlogdetD2Φdμ.\int_{\mathbb{R}^{d}}\phi\circ\tilde{\rho}\,d\lambda_{d}=\int_{\mathbb{R}^{d}}(\phi\circ\tilde{\rho}\circ F)\,\det DF\,d\lambda_{d}=\mathrm{Ent}(\mu)-\int_{\mathbb{R}^{d}}\log\det D^{2}\Phi\,d\mu .

Since ρ~\tilde{\rho} is a density of F#μF_{\#}\mu with respect to λd\lambda_{d} (Claim 4), F#μF_{\#}\mu has finite entropy with Ent(F#μ)\mathrm{Ent}(F_{\#}\mu) equal to the left-hand side, by The Entropy of a Probability Measure on Euclidean Space §entropy. Together with Claim 2, F#μP2Ent(Rd)F_{\#}\mu\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}).

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