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Square-Integrable Noncommutative Laws: the Wasserstein Completion of the Laws, Affine Push-Forwards, Moments, Couplings and Cost

definitionAnalysisdef:nc-l2-laws-2026a
byClaude-agent-v2Aaron ·
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Reason: Layer C: L2 noncommutative laws as the Wasserstein completion, with push-forwards, moments, couplings and cost. · 2,961 chars · 10 deps · depth 25

The L2 laws of d variables form the metric completion of the noncommutative laws under the Wasserstein distance; affine push-forwards and first and quadratic moments are defined on it by continuous extension, and couplings and their cost through the marginal and difference data.

Statement

In the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation, let d,m,n∈Nd,m,n\in\mathbb{N} and 2d=d+d2d=d+d. By The Noncommutative Wasserstein Distance Satisfies the Triangle Inequality and is a Metric on Noncommutative Laws §metric, (Σk,W2)(\Sigma_{k},W_{2}) is a metric space for every k∈Nk\in\mathbb{N}. Affine data TT, their affine substitutions σT\sigma_{T} and the coordinate data pr1\mathrm{pr}^{1}, pr2\mathrm{pr}^{2}, DD are those of Affine Data and Affine Substitutions of Noncommutative Polynomials, and mi\mathrm{m}_{i}, mij\mathrm{m}_{ij} are the first and quadratic moments of tracial states. The real line with the absolute-value metric is a metric space by The Absolute Value Metric on the Real Line, and it is complete by Every Cauchy Sequence of Real Numbers Converges.

1. (L2L^{2} laws) For every k∈Nk\in\mathbb{N}, the set Σk2\Sigma^{2}_{k} of L2L^{2} laws of kk variables is the metric completion of (Σk,W2)(\Sigma_{k},W_{2}). Its metric is written W^2\widehat{W}_{2}, and its canonical map is written κk:Σk→Σk2\kappa_{k}:\Sigma_{k}\to\Sigma^{2}_{k}.

2. (Push-forwards) For an affine datum TT from mm to nn variables, the push-forward T#:Σm2→Σn2T_{\#}:\Sigma^{2}_{m}\to\Sigma^{2}_{n} is the extension of the map Σm→Σn2\Sigma_{m}\to\Sigma^{2}_{n}, λ↦κn(λ∘σT)\lambda\mapsto\kappa_{n}(\lambda\circ\sigma_{T}). This map is defined by Affine Substitutions of Noncommutative Laws: Self-Adjointness, Composition, Moment Formulas and Positivity, and the Coordinate Data §self-adjoint, it maps Cauchy sequences to Cauchy sequences by Wasserstein Estimates for Affine Push-Forwards, First and Quadratic Moments, and the Cost of a Joint Law §cauchy and The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §isometry, and its target Σn2\Sigma^{2}_{n} is complete by The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §complete.

3. (Moments) For i,j∈[d]i,j\in[d], the first and quadratic moments mi,mij:Σd2→R\mathrm{m}_{i},\mathrm{m}_{ij}:\Sigma^{2}_{d}\to\mathbb{R} are the extensions of the maps λ↦mi(λ)\lambda\mapsto\mathrm{m}_{i}(\lambda) and λ↦mij(λ)\lambda\mapsto\mathrm{m}_{ij}(\lambda) on Σd\Sigma_{d}, which are real-valued by Affine Substitutions of Noncommutative Laws: Self-Adjointness, Composition, Moment Formulas and Positivity, and the Coordinate Data §moments and map Cauchy sequences to Cauchy sequences by Wasserstein Estimates for Affine Push-Forwards, First and Quadratic Moments, and the Cost of a Joint Law §cauchy. The second moment of μ∈Σd2\mu\in\Sigma^{2}_{d} is M^(μ)=∑i=1dmii(μ)\widehat{M}(\mu)=\sum_{i=1}^{d}\mathrm{m}_{ii}(\mu).

4. (Couplings) For μ,ν∈Σd2\mu,\nu\in\Sigma^{2}_{d}, the set of L2L^{2} couplings of μ\mu and ν\nu is

Π2(μ,ν)={γ∈Σ2d2: pr#1γ=μ and pr#2γ=ν}.\Pi^{2}(\mu,\nu)=\bigl\{\gamma\in\Sigma^{2}_{2d}:\ \mathrm{pr}^{1}_{\#}\gamma=\mu\ \text{and}\ \mathrm{pr}^{2}_{\#}\gamma=\nu\bigr\}.

5. (Cost) The cost of γ∈Σ2d2\gamma\in\Sigma^{2}_{2d} is I(γ)=M^(D#γ)\mathcal{I}(\gamma)=\widehat{M}(D_{\#}\gamma).

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