TheoremBase

Differentiability of a Function on the Wasserstein Space Along Couplings, and Its Gradient

A function on the Wasserstein space is differentiable along couplings at a measure if its increment is the displacement pairing of a square-integrable vector field along every coupling of small cost, up to an error of smaller order; that field is the gradient.

Statement

In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation, let φ:P2(Rd)→R\varphi:\mathcal{P}_{2}(\mathbb{R}^{d})\to\mathbb{R} and let μ∈P2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}). Let L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) be the space of square-integrable vector fields against μ\mu, let Π(μ,ν)\Pi(\mu,\nu) and II be the couplings and the quadratic cost, and let J(η,π)\mathcal{J}(\eta,\pi) be the displacement pairing of η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}) along π∈Π(μ,ν)\pi\in\Pi(\mu,\nu).

1. (Differentiability along couplings) Let η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}). The function φ\varphi is differentiable along couplings at μ\mu with gradient η\eta if for every ε∈R\varepsilon\in\mathbb{R} with 0<ε0<\varepsilon there is θ∈R\theta\in\mathbb{R} with 0<θ0<\theta such that

∣φ(ν)−φ(μ)−J(η,π)∣≤ε I(π)\bigl|\varphi(\nu)-\varphi(\mu)-\mathcal{J}(\eta,\pi)\bigr|\le\varepsilon\,\sqrt{I(\pi)}

for every ν∈P2(Rd)\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}) and every π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) with I(π)<θ2I(\pi)<\theta^{2}. The function φ\varphi is differentiable along couplings at μ\mu if there is an η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}) with this property.

2. (The gradient along couplings) Suppose that φ\varphi is differentiable along couplings at μ\mu. Then exactly one η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}) has the property of clause 1. Indeed, one exists by that hypothesis. Suppose η\eta and η′\eta' both have it and let ε∈R\varepsilon\in\mathbb{R} be positive, so that ε⋅2−1\varepsilon\cdot2^{-1} is positive by claim 8 of Elementary Order Arithmetic in an Ordered Field. Let θ\theta and θ′\theta' be as in clause 1 for η\eta and for η′\eta' respectively, with ε⋅2−1\varepsilon\cdot2^{-1} there in place of ε\varepsilon, and let θ′′=min⁡{θ,θ′}\theta''=\min\{\theta,\theta'\} be their minimum, which is positive because it equals θ\theta or θ′\theta' by claim 2 of Elementary Properties of the Minimum of Two Elements. Let ν∈P2(Rd)\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}) and π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) satisfy I(π)<(θ′′)2I(\pi)<(\theta'')^{2}. Since θ′′≤θ\theta''\le\theta and θ′′≤θ′\theta''\le\theta' by claim 1 of that lemma, and both sides of each of these inequalities are nonnegative, claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives (θ′′)2≤θ2(\theta'')^{2}\le\theta^{2} and (θ′′)2≤(θ′)2(\theta'')^{2}\le(\theta')^{2}, whence I(π)<θ2I(\pi)<\theta^{2} and I(π)<(θ′)2I(\pi)<(\theta')^{2} by the mixed transitivity of claim 2 of Elementary Order Arithmetic in an Ordered Field. Both estimates of clause 1 are therefore available at π\pi, and, by the linearity of the displacement pairing (The Displacement Pairing of a Square-Integrable Vector Field Along a Coupling (iii), applied with a=1a=1 and b=−1b=-1),

J(η−η′,π)=(φ(ν)−φ(μ)−J(η′,π))−(φ(ν)−φ(μ)−J(η,π)),\mathcal{J}(\eta-\eta',\pi)=\bigl(\varphi(\nu)-\varphi(\mu)-\mathcal{J}(\eta',\pi)\bigr)-\bigl(\varphi(\nu)-\varphi(\mu)-\mathcal{J}(\eta,\pi)\bigr),

so that the triangle inequality of claim 5 of Properties of the Absolute Value in an Ordered Field, together with the symmetry of the absolute value (claim 2 there), bounds ∣J(η−η′,π)∣|\mathcal{J}(\eta-\eta',\pi)| by ε⋅2−1I(π)+ε⋅2−1I(π)\varepsilon\cdot2^{-1}\sqrt{I(\pi)}+\varepsilon\cdot2^{-1}\sqrt{I(\pi)}, which equals εI(π)\varepsilon\sqrt{I(\pi)} by the distributive law of Field and the halving identity of claim 8 of Elementary Order Arithmetic in an Ordered Field. Thus

∣J(η−η′,π)∣≤ε I(π).\bigl|\mathcal{J}(\eta-\eta',\pi)\bigr|\le\varepsilon\,\sqrt{I(\pi)} .

So η−η′\eta-\eta' satisfies the hypothesis of A Square-Integrable Vector Field Whose Displacement Pairings Vanish to First Order is Zero, whence η−η′\eta-\eta' is the zero element by A Square-Integrable Vector Field Whose Displacement Pairings Vanish to First Order is Zero (i) and η=η′\eta=\eta'. This unique η\eta is written ∇φ(μ)\nabla\varphi(\mu) and called the gradient along couplings of φ\varphi at μ\mu.

Citations

Loading…

Dependencies

Loading…

Related

0 relations

Curated associations between results. These are editable and subjective — they do not replace the dependency graph, which is derived from the references in the text.

No relations recorded yet.

Comments

Log in to comment.

Loading…