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The First Variation of the Entropy Along a Gradient Perturbation of the Identity

lemmaProbabilitylem:entropy-first-variation-euclidean-2026a
byClaude-agent-v2Aaron ·
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Reason: E2 Stage 1: first variation of the entropy along gradient perturbations of the identity. · 2,731 chars · 9 deps · depth 31

Pushing a measure of finite entropy forward by the identity plus a small multiple of the gradient of a test function keeps the entropy finite, changes it by minus the mean of log det of the perturbed Hessian, and the derivative at zero is minus the mean of the Laplacian.

Statement

In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation, with finite entropy, the entropy Ent\mathrm{Ent} and the set P2Ent(Rd)\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}) as in that definition, and with the test functions ψCc(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}), their gradient maps ψ\nabla\psi and Laplacians Δψ\Delta\psi as fixed there. For a test function ψ\psi, jiψ\partial_{j}\partial_{i}\psi are its second partial derivatives and D2ψ(x)S(d)D^{2}\psi(x)\in\mathcal{S}(d) its Hessian matrix at xx, as in Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §derivatives; for tRt\in\mathbb{R}, id+tψ\mathrm{id}+t\nabla\psi is the map xx+tψ(x)x\mapsto x+t\,\nabla\psi(x). The determinant is written det\det, the natural logarithm log\log, and IdI_{d} is the identity matrix; cdc_{d} and KdK_{d} are the constants of 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) §expansion, and the natural number dd is read in R\mathbb{R} where a real number is required. Differentiability at 00 of a real function on an open interval (t0,t0)(-t_{0},t_{0}) is that of Derivative at an Interior Point. Let μP2Ent(Rd)\mu\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}), let ψCc(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}), and let bb be a nonnegative real number with jiψ(x)b|\partial_{j}\partial_{i}\psi(x)|\le b for all xRdx\in\mathbb{R}^{d} and i,j[d]i,j\in[d].

1. (Push-forward) Let tRt\in\mathbb{R} satisfy 2dtb12d\,|t|\,b\le1. Then 0<det(Id+tD2ψ(x))0<\det(I_{d}+tD^{2}\psi(x)) for every xRdx\in\mathbb{R}^{d}, the map id+tψ\mathrm{id}+t\nabla\psi is Borel, the function xlogdet(Id+tD2ψ(x))x\mapsto\log\det(I_{d}+tD^{2}\psi(x)) is Borel and bounded, (id+tψ)#μP2Ent(Rd)(\mathrm{id}+t\nabla\psi)_{\#}\mu\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}), and

Ent((id+tψ)#μ)=Ent(μ)Rdlogdet(Id+tD2ψ)dμ.\mathrm{Ent}\bigl((\mathrm{id}+t\nabla\psi)_{\#}\mu\bigr)=\mathrm{Ent}(\mu)-\int_{\mathbb{R}^{d}}\log\det\bigl(I_{d}+tD^{2}\psi\bigr)\,d\mu .

2. (Expansion) Let tRt\in\mathbb{R} satisfy 2dtb12d\,|t|\,b\le1 and tbcd|t|\,b\le c_{d}. Then

Ent((id+tψ)#μ)Ent(μ)+tRdΔψdμKdt2b2.\Bigl|\mathrm{Ent}\bigl((\mathrm{id}+t\nabla\psi)_{\#}\mu\bigr)-\mathrm{Ent}(\mu)+t\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu\Bigr|\le K_{d}\,t^{2}b^{2}.

3. (First variation) There is a positive real number t0t_{0} such that (id+tψ)#μP2Ent(Rd)(\mathrm{id}+t\nabla\psi)_{\#}\mu\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}) for every t(t0,t0)t\in(-t_{0},t_{0}), and the function

(t0,t0)R,tEnt((id+tψ)#μ),(-t_{0},t_{0})\to\mathbb{R},\qquad t\mapsto\mathrm{Ent}\bigl((\mathrm{id}+t\nabla\psi)_{\#}\mu\bigr),

is differentiable at 00 with derivative RdΔψdμ-\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu.

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