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The Free Product of Two Noncommutative Laws: Existence, Uniqueness, Norm Bound, Substitutions and Weak-Star Continuity

Two noncommutative laws have exactly one free joint law with them as marginals, their free product; it keeps a common norm bound, is compatible with substitutions in each group and with swapping the groups, and depends weak-star continuously on the factors.

Statement

In the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation, let m,n∈Nm,n\in\mathbb{N}, and let ι1:Pm→Pm+n\iota^{1}:\mathcal{P}_{m}\to\mathcal{P}_{m+n}, ι2:Pn→Pm+n\iota^{2}:\mathcal{P}_{n}\to\mathcal{P}_{m+n} and freeness be as in Freeness of Two Groups of Variables under a Noncommutative Law §free, for the split of m+nm+n variables into the first mm and the last nn (and likewise for any other split named below). Marginals of laws, and laws obtained from a law by substituting a tuple of self-adjoint polynomials, are laws by Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §law; the tuples substituted below are self-adjoint by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §self-adjoint and Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §adjoint.

1. (Free product) For all α∈Σm\alpha\in\Sigma_{m} and β∈Σn\beta\in\Sigma_{n} there is exactly one free law γ∈Σm+n\gamma\in\Sigma_{m+n} with γ∘ι1=α\gamma\circ\iota^{1}=\alpha and γ∘ι2=β\gamma\circ\iota^{2}=\beta. It is written α⋆β\alpha\star\beta and called the free product of α\alpha and β\beta.

2. (Norm bound) If R>0R>0 is real, α∈Σm,R\alpha\in\Sigma_{m,R} and β∈Σn,R\beta\in\Sigma_{n,R}, then α⋆β∈Σm+n,R\alpha\star\beta\in\Sigma_{m+n,R}.

3. (Substitutions) Let m′,n′∈Nm',n'\in\mathbb{N}, let aa be an m′m'-tuple in Pm,sa\mathcal{P}_{m,\mathrm{sa}}, let bb be an n′n'-tuple in Pn,sa\mathcal{P}_{n,\mathrm{sa}}, and let c=(ι1(a1),…,ι1(am′),ι2(b1),…,ι2(bn′))c=(\iota^{1}(a_{1}),\dots,\iota^{1}(a_{m'}),\iota^{2}(b_{1}),\dots,\iota^{2}(b_{n'})), an (m′+n′)(m'+n')-tuple in Pm+n\mathcal{P}_{m+n}. Then for all α∈Σm\alpha\in\Sigma_{m} and β∈Σn\beta\in\Sigma_{n},

(α⋆β)∘σc=(α∘σa)⋆(β∘σb),(\alpha\star\beta)\circ\sigma_{c}=(\alpha\circ\sigma_{a})\star(\beta\circ\sigma_{b}),

the right side being the free product for the split of m′+n′m'+n' variables into the first m′m' and the last n′n'.

4. (Symmetry) For all α∈Σm\alpha\in\Sigma_{m} and β∈Σn\beta\in\Sigma_{n}, (α⋆β)∘σs=β⋆α(\alpha\star\beta)\circ\sigma_{s}=\beta\star\alpha, where s=(xm+1,…,xm+n,x1,…,xm)s=(x_{m+1},\dots,x_{m+n},x_{1},\dots,x_{m}) and the right side is the free product for the split of n+mn+m variables into the first nn and the last mm.

5. (Weak-star continuity) Let R>0R>0 be real, and let (αk)k∈N(\alpha_{k})_{k\in\mathbb{N}} in Σm,R\Sigma_{m,R} and (βk)k∈N(\beta_{k})_{k\in\mathbb{N}} in Σn,R\Sigma_{n,R} converge weak-star to α∈Σm\alpha\in\Sigma_{m} and β∈Σn\beta\in\Sigma_{n}. Then αk⋆βk→α⋆β\alpha_{k}\star\beta_{k}\to\alpha\star\beta weak-star.

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