TheoremBase

The Torus Displacement Pairing: Linearity, the Cost Bound, and Vanishing of a Field with First-Order Small Pairings

The torus displacement pairing is linear in the field and bounded by the norm of the field times the square root of the torus cost; a field whose pairings along all couplings of small cost are small relative to the square root of the cost is zero.

Statement

In the setting of Optimal Transport on the Flat Torus: Standing Notation, let μ∈P(Td)\mu\in\mathcal{P}(\mathbb{T}^{d}), let L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) and ∥⋅∥μ\lVert\cdot\rVert_{\mu} be as in Optimal Transport on the Flat Torus: Standing Notation §fields, and let JT\mathcal{J}_{\mathbb{T}} be the torus displacement pairing. Then the following hold.

1. (Linearity) For ν∈P(Td)\nu\in\mathcal{P}(\mathbb{T}^{d}), γ∈Π(μ,ν)\gamma\in\Pi(\mu,\nu), η,η′∈L2(μ;Rd)\eta,\eta'\in L^{2}(\mu;\mathbb{R}^{d}) and real a,ba,b: JT(aη+bη′,γ)=a JT(η,γ)+b JT(η′,γ)\mathcal{J}_{\mathbb{T}}(a\eta+b\eta',\gamma)=a\,\mathcal{J}_{\mathbb{T}}(\eta,\gamma)+b\,\mathcal{J}_{\mathbb{T}}(\eta',\gamma).

2. (Cost bound) For ν∈P(Td)\nu\in\mathcal{P}(\mathbb{T}^{d}), γ∈Π(μ,ν)\gamma\in\Pi(\mu,\nu) and η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}): ∣JT(η,γ)∣≤∥η∥μIT(γ)|\mathcal{J}_{\mathbb{T}}(\eta,\gamma)|\le\lVert\eta\rVert_{\mu}\sqrt{I_{\mathbb{T}}(\gamma)}.

3. (Vanishing) Let η∈L2(μ;Rd)\eta\in L^{2}(\mu;\mathbb{R}^{d}), and suppose that for every real ε>0\varepsilon>0 there is a real θ>0\theta>0 such that ∣JT(η,γ)∣≤εIT(γ)|\mathcal{J}_{\mathbb{T}}(\eta,\gamma)|\le\varepsilon\sqrt{I_{\mathbb{T}}(\gamma)} for every ν∈P(Td)\nu\in\mathcal{P}(\mathbb{T}^{d}) and every γ∈Π(μ,ν)\gamma\in\Pi(\mu,\nu) with IT(γ)<θ2I_{\mathbb{T}}(\gamma)<\theta^{2}. Then η\eta is the zero element of L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}).

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