For a bounded plan at a bounded law, the coupling test function built from a differentiable gauge with vanishing derivative at zero and a quadratic weight is attained by a maximising coupling, is Wasserstein-continuous on bounded laws, and admits an explicit plan subjet read off from a maximising coupling; when small displacements pay little momentum it vanishes at the base law, and along laws converging to the base law the maximising couplings collapse and the subjet momenta converge to the plan momenta.
h(t)−h(s)−h′(s)(t−s)≤η∣t−s∣for every real t≥0 with ∣t−s∣<rη,
that h′(0)=0, and that h′(s)→0 as s→0: for every real η>0 there is a real rh>0 with ∣h′(s)∣<η whenever 0≤s<rh. Write Φ=Φκ2d(π)h,θ:Σd2→R for the coupling test function of κ2d(π) with gauge h and weight θ, and, for λ∈Σd2, C(λ)=Cκ2d(π)(λ) for the set of couplings of the plan κ2d(π) with λ, with the displacement and momentum pairings(γ) and p(γ) of γ∈C(λ). For ν∈Σd,r, a maximising coupling for ν is a γ∈C(κd(ν)) with Φ(κd(ν))=p(γ)−h(s(γ))−θs(γ)2.
1. (Maximising couplings) For every ν∈Σd,r there is a maximising coupling for ν.
4. (Localisation) Let r0>0 be real with θr0≥2∣π∣mom, and suppose that p(γ)≤21h(s(γ)) for every γ∈C(κd(μ)) with s(γ)<r0. Then Φ(κd(μ))=0.
5. (Convergence) Let r0>0 be real with θr0≥2∣π∣mom, suppose that p(γ)≤21h(s(γ)) for every γ∈C(κd(μ)) with s(γ)<r0, let (νn)n∈N be a sequence in Σd,r such that the real sequence (W2(νn,μ))n∈N converges to 0, and for every n∈N let γn be a maximising coupling for νn. Then the real sequences (s(γn))n∈N and (Φ(κd(νn)))n∈Nconverge to 0. Moreover, if for every n∈N, (Xn,Pn,Xn′) is a triple of L2d-tuples of a tracial W*-probability space (Hn,Mn,Ωn) with law(Xn,Pn,Xn′)=γn and Sn is defined from Xn,Pn,Xn′ and s(γn)=∥Xn′−Xn∥2 as S is defined from X,P,X′ and s in clause 3, then the real sequence (∥Sn−Pn∥2)n∈N converges to 0.
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