TheoremBase

Everything is transported to a random vector with the given law on the rich space: a translation becomes an added constant class, a gradient displacement an added multiple of the composed gradient field, and the Frechet estimate for the lift, divided by the increment, gives the derivative at time zero.

Proof

Each result cited is universally quantified over the data in its own statement.

By The Wasserstein Distance and the Mean-Square Distance of Random Vectors (iii) there is an X∈L2(Ω;Rd)X\in L^{2}(\Omega;\mathbb{R}^{d}) with L(X)=μ\mathcal{L}(X)=\mu; fix one, and let Φ=φ∘Λ\Phi=\varphi\circ\Lambda be the lift of φ\varphi.

Claim 1. Let a∈Rda\in\mathbb{R}^{d}. By The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation (vi), L(X+ca)=(τa)#L(X)=(τa)#μ\mathcal{L}(X+c_{a})=(\tau_{a})_{\#}\mathcal{L}(X)=(\tau_{a})_{\#}\mu and ∥ca∥L2=∥a∥\lVert c_{a}\rVert_{L^{2}}=\lVert a\rVert. Since X+ca∈L2(Ω;Rd)X+c_{a}\in L^{2}(\Omega;\mathbb{R}^{d}), its law belongs to P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations (ii), so (τa)#μ∈P2(Rd)(\tau_{a})_{\#}\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}). Moreover (X+ca)−X=(X+ca)+(−X)=ca+(X+(−X))=ca(X+c_{a})-X=(X+c_{a})+(-X)=c_{a}+\bigl(X+(-X)\bigr)=c_{a}, by claim 2 of Elementary Identities in a Vector Space for the notation and the commutativity, associativity, inverse and identity axioms of the vector space L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}), so The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation (v) gives

W2((τa)#μ,μ)=W2(L(X+ca),L(X))≤∥(X+ca)−X∥L2=∥ca∥L2=∥a∥.W_{2}\bigl((\tau_{a})_{\#}\mu,\mu\bigr)=W_{2}\bigl(\mathcal{L}(X+c_{a}),\mathcal{L}(X)\bigr)\le\lVert (X+c_{a})-X\rVert_{L^{2}}=\lVert c_{a}\rVert_{L^{2}}=\lVert a\rVert .

Claim 2. Let ψ∈Cc∞(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}) and let t0∈Rt_{0}\in\mathbb{R} be positive; write Gt=id+t ∇ψG_{t}=\mathrm{id}+t\,\nabla\psi and g(t)=φ((Gt)#μ)g(t)=\varphi\bigl((G_{t})_{\#}\mu\bigr) for t∈(−t0,t0)t\in(-t_{0},t_{0}). Let Z=∇ψ∘X∈L2(Ω;Rd)Z=\nabla\psi\circ X\in L^{2}(\Omega;\mathbb{R}^{d}) be the composition of the class of ∇ψ\nabla\psi in L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) with XX; by that clause ∥Z∥L2=∥∇ψ∥μ\lVert Z\rVert_{L^{2}}=\lVert\nabla\psi\rVert_{\mu}.

For t∈Rt\in\mathbb{R} the map GtG_{t} is Borel by The Push-Forward of a Probability Measure with Finite Second Moment by the Identity Perturbed along the Gradient of a Test Function: Borel, Finite Second Moment, the Diagonal Coupling and the Wasserstein Bound (i), so L(Gt∘X)=(Gt)#L(X)=(Gt)#μ\mathcal{L}(G_{t}\circ X)=(G_{t})_{\#}\mathcal{L}(X)=(G_{t})_{\#}\mu by Random Vectors: Coordinates, Functions, Pairs and Almost-Sure Equality (ii). A representative of Gt∘XG_{t}\circ X takes the value X(ω)+t ∇ψ(X(ω))X(\omega)+t\,\nabla\psi(X(\omega)) at ω∈Ω\omega\in\Omega, and, the sum and the real multiple in L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}) being formed pointwise on representatives by Square-Integrable Random Vectors: Coordinates, Operations, Almost Sure Equality and the Mean-Square Form (ii), so does a representative of X+tZX+tZ; the two classes are therefore equal, Gt∘X=X+tZG_{t}\circ X=X+tZ. Hence

g(t)=Φ(X+tZ)(t∈(−t0,t0)).g(t)=\Phi(X+tZ)\qquad\bigl(t\in(-t_{0},t_{0})\bigr).

By condition (a) of Test Functions on the Wasserstein Space: the Intrinsic Gradient and the Translation Hessian (i) and The Classes C1C^1 and C2C^2 on an Open Subset of a Real Inner Product Space (i), Φ\Phi is differentiable at XX with gradient DΦ(X)D\Phi(X), and DΦ(X)=∇φ(μ)∘XD\Phi(X)=\nabla\varphi(\mu)\circ X by condition (b) and Test Functions on the Wasserstein Space: the Intrinsic Gradient and the Translation Hessian (ii). Writing L=⟨∇φ(μ),∇ψ⟩μL=\langle\nabla\varphi(\mu),\nabla\psi\rangle_{\mu}, the preservation of inner products in Composition of a Square-Integrable Vector Field with a Random Vector, and the Lifted Score: Isometry, Norm, Weak Identity and Second-Moment Identity (i) gives

⟨DΦ(X),Z⟩L2=⟨∇φ(μ)∘X,∇ψ∘X⟩L2=L.\langle D\Phi(X),Z\rangle_{L^{2}}=\langle\nabla\varphi(\mu)\circ X,\nabla\psi\circ X\rangle_{L^{2}}=L .

Let ε∈R\varepsilon\in\mathbb{R} be positive and put c=∥Z∥L2c=\lVert Z\rVert_{L^{2}}, so 0≤c0\le c and 0<c+10<c+1 by claim 3 of Elementary Order Arithmetic in an Ordered Field applied to 0<10<1 (claim 6 of that lemma) and 0≤c0\le c. The number ε(c+1)−1\varepsilon(c+1)^{-1} is positive by claims 7 and 5 of that lemma, so Fréchet Differentiability and the Gradient on an Open Subset of a Real Inner Product Space (i) provides a positive ρ∈R\rho\in\mathbb{R} with

∣Φ(X+V)−Φ(X)−⟨DΦ(X),V⟩L2∣≤ε(c+1)−1∥V∥L2for every V∈L2(Ω;Rd) with ∥V∥L2<ρ.\bigl|\Phi(X+V)-\Phi(X)-\langle D\Phi(X),V\rangle_{L^{2}}\bigr|\le\varepsilon(c+1)^{-1}\lVert V\rVert_{L^{2}}\qquad\text{for every }V\in L^{2}(\Omega;\mathbb{R}^{d})\text{ with }\lVert V\rVert_{L^{2}}<\rho .

Let η\eta be the lesser of t0t_{0} and ρ(c+1)−1\rho(c+1)^{-1} (claim 9 of Elementary Order Arithmetic in an Ordered Field), positive because it is one of them, and let h∈Rh\in\mathbb{R} satisfy 0<∣h∣<η0<|h|<\eta and h∈(−t0,t0)h\in(-t_{0},t_{0}). Then, by Elementary Identities in a Real Inner Product Space (iv) and claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative multiplier ∣h∣|h|, and by claim 10 of Elementary Order Arithmetic in an Ordered Field with the positive multiplier c+1c+1,

∥hZ∥L2=∣h∣ c≤∣h∣ (c+1)<η (c+1)≤ρ.\lVert hZ\rVert_{L^{2}}=|h|\,c\le|h|\,(c+1)<\eta\,(c+1)\le\rho .

Taking V=hZV=hZ and using ⟨DΦ(X),hZ⟩L2=h L\langle D\Phi(X),hZ\rangle_{L^{2}}=h\,L (Elementary Identities in a Real Inner Product Space (i)) therefore gives

∣g(h)−g(0)−h L∣≤ε(c+1)−1∣h∣ c.\bigl|g(h)-g(0)-h\,L\bigr|\le\varepsilon(c+1)^{-1}|h|\,c .

Now g(h)−g(0)h−L=(g(h)−g(0)−h L)h−1\frac{g(h)-g(0)}{h}-L=\bigl(g(h)-g(0)-h\,L\bigr)h^{-1}, and ∣h∣ ∣h−1∣=∣h h−1∣=∣1∣=1|h|\,|h^{-1}|=|h\,h^{-1}|=|1|=1 by claim 4 of Properties of the Absolute Value in an Ordered Field and Absolute Value in an Ordered Field, so multiplying the last display by ∣h∣−1|h|^{-1}, nonnegative by claim 7 of Elementary Order Arithmetic in an Ordered Field, yields by claim 5 of Elementary Arithmetic in an Ordered Field

∣g(h)−g(0)h−L∣≤ε(c+1)−1c<ε,\left|\frac{g(h)-g(0)}{h}-L\right|\le\varepsilon(c+1)^{-1}c<\varepsilon ,

the final inequality because c<c+1c<c+1 gives c (c+1)−1<1c\,(c+1)^{-1}<1 and hence ε(c+1)−1c<ε\varepsilon(c+1)^{-1}c<\varepsilon, by claim 10 of Elementary Order Arithmetic in an Ordered Field with the positive multipliers (c+1)−1(c+1)^{-1} and ε\varepsilon. Since ε\varepsilon was an arbitrary positive real number, gg is differentiable at 00 with g′(0)=Lg'(0)=L by Derivative of a Real Function on an Interval, 00 lying in (−t0,t0)(-t_{0},t_{0}) because −t0<−0=0<t0-t_{0}<-0=0<t_{0} by claim 4 of Elementary Order Arithmetic in an Ordered Field and being interior to it by Basic Facts about Intervals of the Real Line (iv).

Claim 3. The function a↦φ((τa)#μ)a\mapsto\varphi\bigl((\tau_{a})_{\#}\mu\bigr) is the function ϕX\phi_{X} with ϕX(a)=Φ(X+ca)\phi_{X}(a)=\Phi(X+c_{a}) attached to Φ\Phi at XX in The Translation Laplacian of a Function on the Space of Square-Integrable Random Vectors (i), because L(X+ca)=(τa)#μ\mathcal{L}(X+c_{a})=(\tau_{a})_{\#}\mu by The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation (vi) and Φ=φ∘Λ\Phi=\varphi\circ\Lambda. By condition (c) of Test Functions on the Wasserstein Space: the Intrinsic Gradient and the Translation Hessian (i) it is of class C2C^{2} on Rd\mathbb{R}^{d}, and its Hessian matrix at 0Rd0_{\mathbb{R}^{d}} is Hφ(μ)H_{\varphi}(\mu) by Test Functions on the Wasserstein Space: the Intrinsic Gradient and the Translation Hessian (iii), which also shows that this matrix does not depend on the choice of XX.

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