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.
1. (Linearity) For ν∈P(Td), γ∈Π(μ,ν), η,η′∈L2(μ;Rd) and real a,b: JT(aη+bη′,γ)=aJT(η,γ)+bJT(η′,γ).
2. (Cost bound) For ν∈P(Td), γ∈Π(μ,ν) and η∈L2(μ;Rd): ∣JT(η,γ)∣≤∥η∥μIT(γ).
3. (Vanishing) Let η∈L2(μ;Rd), and suppose that for every real ε>0 there is a real θ>0 such that ∣JT(η,γ)∣≤εIT(γ) for every ν∈P(Td) and every γ∈Π(μ,ν) with IT(γ)<θ2. Then η is the zero element of L2(μ;Rd).
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