Each result cited is universally quantified over the data in its own statement. Write B ( x ) = D 2 ψ ( x ) B(x)=D^{2}\psi(x) B ( x ) = D 2 ψ ( x ) for x ∈ R d x\in\mathbb{R}^{d} x ∈ R d and, for t ∈ R t\in\mathbb{R} t ∈ R , μ t = ( i d + t ∇ ψ ) # μ \mu_{t}=(\mathrm{id}+t\nabla\psi)_{\#}\mu μ t = ( id + t ∇ ψ ) # μ .
Step 1 (the potential). Fix t ∈ R t\in\mathbb{R} t ∈ R and let Φ t : R d → R \Phi_{t}:\mathbb{R}^{d}\to\mathbb{R} Φ t : R d → R be Φ t ( x ) = 1 2 ∥ x ∥ 2 + t ψ ( x ) = 1 2 ∑ i = 1 d x i 2 + t ψ ( x ) \Phi_{t}(x)=\tfrac12\lVert x\rVert^{2}+t\psi(x)=\tfrac12\sum_{i=1}^{d}x_{i}^{2}+t\psi(x) Φ t ( x ) = 2 1 ∥ x ∥ 2 + t ψ ( x ) = 2 1 ∑ i = 1 d x i 2 + t ψ ( x ) . Coordinate functions, products, sums and scalar multiples of C 2 C^{2} C 2 functions are C 2 C^{2} C 2 by Constants, Coordinate Functions, Sums and Products of C k C^k C k Functions on a Euclidean Open Set , and ψ \psi ψ is smooth, hence C 2 C^{2} C 2 (Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient ); so Φ t \Phi_{t} Φ t is of class C 2 C^{2} C 2 on R d \mathbb{R}^{d} R d , with
∂ i Φ t ( x ) = x i + t ∂ i ψ ( x ) , ∂ j ∂ i Φ t ( x ) = δ i j + t ∂ j ∂ i ψ ( 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), ∂ i Φ t ( x ) = x i + t ∂ i ψ ( x ) , ∂ j ∂ i Φ t ( x ) = δ ij + t ∂ j ∂ i ψ ( x ) ,
where δ i j \delta_{ij} δ ij is the entry of I d I_{d} I d in row i i i and column j j j . Thus the gradient map of Φ t \Phi_{t} Φ t is i d + t ∇ ψ \mathrm{id}+t\nabla\psi id + t ∇ ψ and D 2 Φ t ( x ) = I d + t B ( x ) D^{2}\Phi_{t}(x)=I_{d}+tB(x) D 2 Φ t ( x ) = I d + tB ( x ) .
Step 2 (pinching). Let x , v ∈ R d x,v\in\mathbb{R}^{d} x , v ∈ R d . Since ∣ B i j ( x ) ∣ ≤ b |B_{ij}(x)|\le b ∣ B ij ( x ) ∣ ≤ b ,
∣ v T B ( x ) v ∣ = ∣ ∑ i , j = 1 d B i j ( x ) v i v j ∣ ≤ b ( ∑ i = 1 d ∣ v i ∣ ) 2 ≤ b d ∥ v ∥ 2 , |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}, ∣ v T B ( x ) v ∣ = i , j = 1 ∑ d B ij ( x ) v i v j ≤ b ( i = 1 ∑ d ∣ v i ∣ ) 2 ≤ b d ∥ v ∥ 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 ( ∣ v 1 ∣ , … , ∣ v d ∣ ) (|v_{1}|,\dots,|v_{d}|) ( ∣ v 1 ∣ , … , ∣ v d ∣ ) and ( 1 , … , 1 ) (1,\dots,1) ( 1 , … , 1 ) . Hence, if 2 d ∣ t ∣ b ≤ 1 2d|t|b\le1 2 d ∣ t ∣ b ≤ 1 , then v T ( I d + t B ( x ) ) v = ∥ v ∥ 2 + t v T B ( x ) v v^{\mathsf T}(I_{d}+tB(x))v=\lVert v\rVert^{2}+t\,v^{\mathsf T}B(x)v v T ( I d + tB ( x )) v = ∥ v ∥ 2 + t v T B ( x ) v lies between 1 2 ∥ v ∥ 2 \tfrac12\lVert v\rVert^{2} 2 1 ∥ v ∥ 2 and 3 2 ∥ v ∥ 2 \tfrac32\lVert v\rVert^{2} 2 3 ∥ v ∥ 2 ; that is, 1 2 I d ⪯ D 2 Φ t ( x ) ⪯ 3 2 I d \tfrac12I_{d}\preceq D^{2}\Phi_{t}(x)\preceq\tfrac32I_{d} 2 1 I d ⪯ D 2 Φ t ( x ) ⪯ 2 3 I d in the positive semidefinite ordering .
Claim 1. Let 2 d ∣ t ∣ b ≤ 1 2d|t|b\le1 2 d ∣ t ∣ b ≤ 1 . By Step 2 and Determinants of Positive Definite Matrices: Positivity, the Bound log det A ≤ t r A − d \log\det A\le\mathrm{tr}\,A-d log det A ≤ tr A − d , Bounds under Pinching, and the Expansion of det ( I + t B ) \det(I+tB) det ( I + tB ) §pinching (with ε = 1 2 \varepsilon=\tfrac12 ε = 2 1 , L = 3 2 L=\tfrac32 L = 2 3 ) the matrix I d + t B ( x ) I_{d}+tB(x) I d + tB ( x ) is positive definite, so 0 < det ( I d + t B ( x ) ) 0<\det(I_{d}+tB(x)) 0 < det ( I d + tB ( x )) by Determinants of Positive Definite Matrices: Positivity, the Bound log det A ≤ t r A − d \log\det A\le\mathrm{tr}\,A-d log det A ≤ tr A − d , Bounds under Pinching, and the Expansion of det ( I + t B ) \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 = Φ t \Phi=\Phi_{t} Φ = Φ t with ε = 1 2 \varepsilon=\tfrac12 ε = 2 1 and L = 3 2 L=\tfrac32 L = 2 3 : its preamble gives that ∇ Φ t = i d + t ∇ ψ \nabla\Phi_{t}=\mathrm{id}+t\nabla\psi ∇ Φ t = id + t ∇ ψ 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 x ↦ log det ( I d + t B ( x ) ) x\mapsto\log\det(I_{d}+tB(x)) x ↦ log det ( I d + tB ( x )) is Borel and bounded, that μ t ∈ P 2 E n t ( R d ) \mu_{t}\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}) μ t ∈ P 2 Ent ( R d ) , and the stated formula.
Claim 2. Let 2 d ∣ t ∣ b ≤ 1 2d|t|b\le1 2 d ∣ t ∣ b ≤ 1 and ∣ t ∣ b ≤ c d |t|b\le c_{d} ∣ t ∣ b ≤ c d . The trace of B ( x ) B(x) B ( x ) is ∑ i ∂ i ∂ i ψ ( x ) = Δ ψ ( x ) \sum_{i}\partial_{i}\partial_{i}\psi(x)=\Delta\psi(x) ∑ i ∂ i ∂ i ψ ( x ) = Δ ψ ( x ) by The Laplacian of a Twice Continuously Differentiable Function §laplacian . Since c d ≤ 1 c_{d}\le1 c d ≤ 1 , Determinants of Positive Definite Matrices: Positivity, the Bound log det A ≤ t r A − d \log\det A\le\mathrm{tr}\,A-d log det A ≤ tr A − d , Bounds under Pinching, and the Expansion of det ( I + t B ) \det(I+tB) det ( I + tB ) §expansion applies with the matrix B ( x ) B(x) B ( x ) , its entry bound taken to be b b b , and this t t t , and gives for every x x x
∣ log det ( I d + t B ( x ) ) − t Δ ψ ( x ) ∣ ≤ K d t 2 b 2 . \bigl|\log\det(I_{d}+tB(x))-t\,\Delta\psi(x)\bigr|\le K_{d}\,t^{2}b^{2}. log det ( I d + tB ( x )) − t Δ ψ ( x ) ≤ K d t 2 b 2 .
Both log det ( I d + t B ) \log\det(I_{d}+tB) log det ( I d + tB ) (Claim 1) and Δ ψ \Delta\psi Δ ψ (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 μ -integrable, so by Claim 1 and claim 2 of Linearity and Monotonicity of the Lebesgue Integral ,
E n t ( μ t ) − E n t ( μ ) + t ∫ R d Δ ψ d μ = − ∫ R d ( log det ( I d + t B ) − t Δ ψ ) d μ , \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, Ent ( μ t ) − Ent ( μ ) + t ∫ R d Δ ψ d μ = − ∫ R d ( log det ( I d + tB ) − t Δ ψ ) d μ ,
whose absolute value is at most ∫ K d t 2 b 2 d μ = K d t 2 b 2 \int K_{d}t^{2}b^{2}\,d\mu=K_{d}t^{2}b^{2} ∫ K d t 2 b 2 d μ = K d t 2 b 2 by monotonicity of the integral (the same theorem) and μ ( R d ) = 1 \mu(\mathbb{R}^{d})=1 μ ( R d ) = 1 .
Claim 3. Let t 0 = 1 t_{0}=1 t 0 = 1 if b = 0 b=0 b = 0 , and otherwise let t 0 t_{0} t 0 be the smaller of ( 2 d b ) − 1 (2db)^{-1} ( 2 d b ) − 1 and c d b − 1 c_{d}b^{-1} c d b − 1 ; in either case t 0 > 0 t_{0}>0 t 0 > 0 , and every t ∈ ( − t 0 , t 0 ) t\in(-t_{0},t_{0}) t ∈ ( − t 0 , t 0 ) satisfies 2 d ∣ t ∣ b ≤ 1 2d|t|b\le1 2 d ∣ t ∣ b ≤ 1 and ∣ t ∣ b ≤ c d |t|b\le c_{d} ∣ t ∣ b ≤ c d . By Claim 1, μ t ∈ P 2 E n t ( R d ) \mu_{t}\in\mathcal{P}_{2}^{\mathrm{Ent}}(\mathbb{R}^{d}) μ t ∈ P 2 Ent ( R d ) for all such t t t ; let F ( t ) = E n t ( μ t ) F(t)=\mathrm{Ent}(\mu_{t}) F ( t ) = Ent ( μ t ) . Since μ 0 = i d # μ = μ \mu_{0}=\mathrm{id}_{\#}\mu=\mu μ 0 = id # μ = μ , Claim 2 gives, for 0 < ∣ t ∣ < t 0 0<|t|<t_{0} 0 < ∣ t ∣ < t 0 ,
∣ F ( t ) − F ( 0 ) t − ( − ∫ R d Δ ψ d μ ) ∣ = ∣ F ( t ) − F ( 0 ) + t ∫ Δ ψ d μ ∣ ∣ t ∣ ≤ K d b 2 ∣ t ∣ . \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|. t F ( t ) − F ( 0 ) − ( − ∫ R d Δ ψ d μ ) = ∣ t ∣ F ( t ) − F ( 0 ) + t ∫ Δ ψ d μ ≤ K d b 2 ∣ t ∣.
Given ε > 0 \varepsilon>0 ε > 0 , the right side is below ε \varepsilon ε whenever 0 < ∣ t ∣ < δ 0<|t|<\delta 0 < ∣ t ∣ < δ , where δ \delta δ is the smaller of t 0 t_{0} t 0 and ε ( K d b 2 + 1 ) − 1 \varepsilon(K_{d}b^{2}+1)^{-1} ε ( K d b 2 + 1 ) − 1 . The point 0 0 0 is an interior point of ( − t 0 , t 0 ) (-t_{0},t_{0}) ( − 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 F F F is differentiable at 0 0 0 with derivative − ∫ R d Δ ψ d μ -\int_{\mathbb{R}^{d}}\Delta\psi\,d\mu − ∫ R d Δ ψ d μ . ■ \blacksquare ■