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

lemmalem:entropy-first-variation-euclidean-2026a
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· 4,514 chars · 12 deps · depth 32 Reason: E2 Stage 1: proof of the first variation of the entropy.

The perturbed map is the gradient of |x|^2/2 + t psi, whose Hessian is pinched between I/2 and 3I/2 for small t, so the push-forward lemma gives the exact entropy change; the log-det expansion bounds its deviation from -t times the mean Laplacian by a multiple of t2t^2, which yields the derivative.

Proof

Each result cited is universally quantified over the data in its own statement. Write B(x)=D2ψ(x)B(x)=D^{2}\psi(x) for xRdx\in\mathbb{R}^{d} and, for tRt\in\mathbb{R}, μt=(id+tψ)#μ\mu_{t}=(\mathrm{id}+t\nabla\psi)_{\#}\mu.

Step 1 (the potential). Fix tRt\in\mathbb{R} and let Φt:RdR\Phi_{t}:\mathbb{R}^{d}\to\mathbb{R} be Φt(x)=12x2+tψ(x)=12i=1dxi2+tψ(x)\Phi_{t}(x)=\tfrac12\lVert x\rVert^{2}+t\psi(x)=\tfrac12\sum_{i=1}^{d}x_{i}^{2}+t\psi(x). Coordinate functions, products, sums and scalar multiples of C2C^{2} functions are C2C^{2} by Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, and ψ\psi is smooth, hence C2C^{2} (Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient); so Φt\Phi_{t} is of class C2C^{2} on Rd\mathbb{R}^{d}, with

iΦt(x)=xi+tiψ(x),jiΦt(x)=δij+tjiψ(x),\partial_{i}\Phi_{t}(x)=x_{i}+t\,\partial_{i}\psi(x),\qquad\partial_{j}\partial_{i}\Phi_{t}(x)=\delta_{ij}+t\,\partial_{j}\partial_{i}\psi(x),

where δij\delta_{ij} is the entry of IdI_{d} in row ii and column jj. Thus the gradient map of Φt\Phi_{t} is id+tψ\mathrm{id}+t\nabla\psi and D2Φt(x)=Id+tB(x)D^{2}\Phi_{t}(x)=I_{d}+tB(x).

Step 2 (pinching). Let x,vRdx,v\in\mathbb{R}^{d}. Since Bij(x)b|B_{ij}(x)|\le b,

vTB(x)v=i,j=1dBij(x)vivjb(i=1dvi)2bdv2,|v^{\mathsf T}B(x)v|=\Bigl|\sum_{i,j=1}^{d}B_{ij}(x)v_{i}v_{j}\Bigr|\le b\Bigl(\sum_{i=1}^{d}|v_{i}|\Bigr)^{2}\le b\,d\,\lVert v\rVert^{2},

the first inequality by the triangle inequality and claim 4 of Properties of the Absolute Value in an Ordered Field, the second by Cauchy-Schwarz Inequality for the Euclidean Dot Product applied to (v1,,vd)(|v_{1}|,\dots,|v_{d}|) and (1,,1)(1,\dots,1). Hence, if 2dtb12d|t|b\le1, then vT(Id+tB(x))v=v2+tvTB(x)vv^{\mathsf T}(I_{d}+tB(x))v=\lVert v\rVert^{2}+t\,v^{\mathsf T}B(x)v lies between 12v2\tfrac12\lVert v\rVert^{2} and 32v2\tfrac32\lVert v\rVert^{2}; that is, 12IdD2Φt(x)32Id\tfrac12I_{d}\preceq D^{2}\Phi_{t}(x)\preceq\tfrac32I_{d} in the positive semidefinite ordering.

Claim 1. Let 2dtb12d|t|b\le1. By Step 2 and 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 (with ε=12\varepsilon=\tfrac12, L=32L=\tfrac32) the matrix Id+tB(x)I_{d}+tB(x) is positive definite, so 0<det(Id+tB(x))0<\det(I_{d}+tB(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. By Steps 1 and 2, The Entropy of the Push-Forward of a Measure by the Gradient of a Twice Continuously Differentiable Function with Pinched Hessian applies to Φ=Φt\Phi=\Phi_{t} with ε=12\varepsilon=\tfrac12 and L=32L=\tfrac32: its preamble gives that Φt=id+tψ\nabla\Phi_{t}=\mathrm{id}+t\nabla\psi is Borel, and The Entropy of the Push-Forward of a Measure by the Gradient of a Twice Continuously Differentiable Function with Pinched Hessian §entropy gives that xlogdet(Id+tB(x))x\mapsto\log\det(I_{d}+tB(x)) is Borel and bounded, that μtP2Ent(Rd)\mu_{t}\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}), and the stated formula.

Claim 2. Let 2dtb12d|t|b\le1 and tbcd|t|b\le c_{d}. The trace of B(x)B(x) is iiiψ(x)=Δψ(x)\sum_{i}\partial_{i}\partial_{i}\psi(x)=\Delta\psi(x) by The Laplacian of a Twice Continuously Differentiable Function §laplacian. Since cd1c_{d}\le1, 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 applies with the matrix B(x)B(x), its entry bound taken to be bb, and this tt, and gives for every xx

logdet(Id+tB(x))tΔψ(x)Kdt2b2.\bigl|\log\det(I_{d}+tB(x))-t\,\Delta\psi(x)\bigr|\le K_{d}\,t^{2}b^{2}.

Both logdet(Id+tB)\log\det(I_{d}+tB) (Claim 1) and Δψ\Delta\psi (The Gradient of a Test Function is Bounded and Square-Integrable, and Its Laplacian Bounded and Integrable, Against Every Probability Measure §laplacian) are bounded Borel functions, hence μ\mu-integrable, so by Claim 1 and claim 2 of Linearity and Monotonicity of the Lebesgue Integral,

Ent(μt)Ent(μ)+tRdΔψdμ=Rd(logdet(Id+tB)tΔψ)dμ,\mathrm{Ent}(\mu_{t})-\mathrm{Ent}(\mu)+t\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu=-\int_{\mathbb{R}^{d}}\bigl(\log\det(I_{d}+tB)-t\,\Delta\psi\bigr)\,d\mu,

whose absolute value is at most Kdt2b2dμ=Kdt2b2\int K_{d}t^{2}b^{2}\,d\mu=K_{d}t^{2}b^{2} by monotonicity of the integral (the same theorem) and μ(Rd)=1\mu(\mathbb{R}^{d})=1.

Claim 3. Let t0=1t_{0}=1 if b=0b=0, and otherwise let t0t_{0} be the smaller of (2db)1(2db)^{-1} and cdb1c_{d}b^{-1}; in either case t0>0t_{0}>0, and every t(t0,t0)t\in(-t_{0},t_{0}) satisfies 2dtb12d|t|b\le1 and tbcd|t|b\le c_{d}. By Claim 1, μtP2Ent(Rd)\mu_{t}\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}) for all such tt; let F(t)=Ent(μt)F(t)=\mathrm{Ent}(\mu_{t}). Since μ0=id#μ=μ\mu_{0}=\mathrm{id}_{\#}\mu=\mu, Claim 2 gives, for 0<t<t00<|t|<t_{0},

F(t)F(0)t(RdΔψdμ)=F(t)F(0)+tΔψdμtKdb2t.\Bigl|\frac{F(t)-F(0)}{t}-\Bigl(-\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu\Bigr)\Bigr|=\frac{\bigl|F(t)-F(0)+t\int\Delta\psi\,d\mu\bigr|}{|t|}\le K_{d}\,b^{2}\,|t|.

Given ε>0\varepsilon>0, the right side is below ε\varepsilon whenever 0<t<δ0<|t|<\delta, where δ\delta is the smaller of t0t_{0} and ε(Kdb2+1)1\varepsilon(K_{d}b^{2}+1)^{-1}. The point 00 is an interior point of (t0,t0)(-t_{0},t_{0}) by Basic Facts about Intervals of the Real Line and Their Interior Points §open-interval, so by Derivative at an Interior Point the function FF is differentiable at 00 with derivative RdΔψdμ-\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu. \blacksquare

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