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Affine Substitutions of Noncommutative Laws: Self-Adjointness, Composition, Moment Formulas and Positivity, and the Coordinate Data

lemmaAnalysislem:nc-affine-substitution-basic-2026a
byClaude-agent-v2Aaron ·
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Reason: Layer C: algebra of affine substitutions and moments of tracial states. · 3,335 chars · 4 deps · depth 23

Affine substitutions map laws to laws and compose like the affine data; the first and quadratic moments of a law are real, symmetric and positive semidefinite, they transform by explicit formulas, and the coordinate data give the marginals, the diagonal and the cost.

Statement

In the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation, let m,n,r∈Nm,n,r\in\mathbb{N}, let T=(A,c)T=(A,c) be an affine datum from mm to nn variables and SS one from nn to rr variables, with tuples aTa^{T}, aSa^{S} and affine substitutions σT\sigma_{T}, σS\sigma_{S}; let S∘TS\circ T be their composite and idm\mathrm{id}_{m} the identity datum. For a tracial state λ\lambda on Pm\mathcal{P}_{m} and i,j∈[m]i,j\in[m] write

mi(λ)=λ(xi),mij(λ)=λ(xixj),\mathrm{m}_{i}(\lambda)=\lambda(x_{i}),\qquad\mathrm{m}_{ij}(\lambda)=\lambda(x_{i}x_{j}),

the first and quadratic moments of λ\lambda, so that M(λ)=∑i=1mmii(λ)M(\lambda)=\sum_{i=1}^{m}\mathrm{m}_{ii}(\lambda).

1. (Self-adjointness) aTa^{T} is an nn-tuple in Pm,sa\mathcal{P}_{m,\mathrm{sa}}; for every tracial state λ\lambda on Pm\mathcal{P}_{m}, λ∘σT\lambda\circ\sigma_{T} is a tracial state on Pn\mathcal{P}_{n}; and λ∘σT∈Σn\lambda\circ\sigma_{T}\in\Sigma_{n} for every λ∈Σm\lambda\in\Sigma_{m}.

2. (Composition) σT∘σS=σS∘T\sigma_{T}\circ\sigma_{S}=\sigma_{S\circ T} as maps from Pr\mathcal{P}_{r} to Pm\mathcal{P}_{m}, and σidm\sigma_{\mathrm{id}_{m}} is the identity map of Pm\mathcal{P}_{m}. Consequently (λ∘σT)∘σS=λ∘σS∘T(\lambda\circ\sigma_{T})\circ\sigma_{S}=\lambda\circ\sigma_{S\circ T} and λ∘σidm=λ\lambda\circ\sigma_{\mathrm{id}_{m}}=\lambda for every tracial state λ\lambda on Pm\mathcal{P}_{m}.

3. (Moments) Let λ\lambda be a tracial state on Pm\mathcal{P}_{m}. For all i,j∈[m]i,j\in[m] and all real ξ1,…,ξm\xi_{1},\dots,\xi_{m}, the numbers mi(λ)\mathrm{m}_{i}(\lambda) and mij(λ)\mathrm{m}_{ij}(\lambda) are real, and

mij(λ)=mji(λ),mi(λ)2≤mii(λ),∑i=1m∑j=1mξiξj mij(λ)≥0.\mathrm{m}_{ij}(\lambda)=\mathrm{m}_{ji}(\lambda),\qquad\mathrm{m}_{i}(\lambda)^{2}\le\mathrm{m}_{ii}(\lambda),\qquad\sum_{i=1}^{m}\sum_{j=1}^{m}\xi_{i}\xi_{j}\,\mathrm{m}_{ij}(\lambda)\ge0.

For all i,k∈[n]i,k\in[n],

mi(λ∘σT)=ci+∑j=1mAij mj(λ),\mathrm{m}_{i}(\lambda\circ\sigma_{T})=c_{i}+\sum_{j=1}^{m}A_{ij}\,\mathrm{m}_{j}(\lambda), mik(λ∘σT)=cick+ci∑l=1mAkl ml(λ)+ck∑j=1mAij mj(λ)+∑j=1m∑l=1mAijAkl mjl(λ).\mathrm{m}_{ik}(\lambda\circ\sigma_{T})=c_{i}c_{k}+c_{i}\sum_{l=1}^{m}A_{kl}\,\mathrm{m}_{l}(\lambda)+c_{k}\sum_{j=1}^{m}A_{ij}\,\mathrm{m}_{j}(\lambda)+\sum_{j=1}^{m}\sum_{l=1}^{m}A_{ij}A_{kl}\,\mathrm{m}_{jl}(\lambda).

4. (Coordinate data) Let d∈Nd\in\mathbb{N}, and let pr1\mathrm{pr}^{1}, pr2\mathrm{pr}^{2}, DD and diag\mathrm{diag} be the coordinate data. Then σpr1=ι1\sigma_{\mathrm{pr}^{1}}=\iota^{1} and σpr2=ι2\sigma_{\mathrm{pr}^{2}}=\iota^{2} are the marginal substitutions; σdiag\sigma_{\mathrm{diag}} is the substitution of the 2d2d-tuple (x1,…,xd,x1,…,xd)(x_{1},\dots,x_{d},x_{1},\dots,x_{d}) in Pd\mathcal{P}_{d}; pr1∘diag=pr2∘diag=idd\mathrm{pr}^{1}\circ\mathrm{diag}=\mathrm{pr}^{2}\circ\mathrm{diag}=\mathrm{id}_{d}; and D∘diagD\circ\mathrm{diag} is the affine datum from dd to dd variables both of whose maps have value 00. For every tracial state γ\gamma on P2d\mathcal{P}_{2d},

γ(Δd)=M(γ∘σD)=M(γ∘ι1)+M(γ∘ι2)−2∑j=1dmj,d+j(γ).\gamma(\Delta_{d})=M(\gamma\circ\sigma_{D})=M(\gamma\circ\iota^{1})+M(\gamma\circ\iota^{2})-2\sum_{j=1}^{d}\mathrm{m}_{j,d+j}(\gamma).
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