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Proof of The Amalgamated Free Product Space: Multilinearity of the Tuple Vectors and the Bounded Left Actions of the Two Tracial Algebras

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· 19,912 chars · 16 deps · depth 25 Reason: G4: proof of multilinearity and the bounded left actions.

Differences of vectors that pair identically with every basis vector are null; this gives multilinearity, balance and the relations case by case, and the bound follows by writing the norm squared of b times the identity minus bb as cc.

Proof

Preliminaries. Let ε∈{1,2}\varepsilon\in\{1,2\}. By Two Noncommutative Laws with a Common Marginal: Standing Notation for Their Amalgamated Free Product §embeddings, Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §homomorphism and Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §expectation (for γ=γε\gamma=\gamma_{\varepsilon}), πε\pi_{\varepsilon} is linear with πε(I)=I\pi_{\varepsilon}(I)=I, πε(ST)=πε(S)πε(T)\pi_{\varepsilon}(ST)=\pi_{\varepsilon}(S)\pi_{\varepsilon}(T) and πε(T∗)=πε(T)∗\pi_{\varepsilon}(T^{*})=\pi_{\varepsilon}(T)^{*}, and EεE_{\varepsilon} is linear with Eε(πε(S) c πε(T))=S Eε(c) TE_{\varepsilon}(\pi_{\varepsilon}(S)\,c\,\pi_{\varepsilon}(T))=S\,E_{\varepsilon}(c)\,T and Eε(πε(T))=TE_{\varepsilon}(\pi_{\varepsilon}(T))=T for S,T∈NS,T\in N and c∈Aεc\in A_{\varepsilon}. All sums, scalar multiples, products and adjoints formed below lie in AεA_{\varepsilon} or NN by The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots §star-algebra, and products of operators distribute over sums and commute with scalar multiples by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations. For c∈Aεc\in A_{\varepsilon} and y∈Ny\in N we record four consequences. (F1) Taking S=IS=I or T=IT=I: Eε(c πε(y))=Eε(c) yE_{\varepsilon}(c\,\pi_{\varepsilon}(y))=E_{\varepsilon}(c)\,y and Eε(πε(y) c)=y Eε(c)E_{\varepsilon}(\pi_{\varepsilon}(y)\,c)=y\,E_{\varepsilon}(c). (F2) Since πε\pi_{\varepsilon} and EεE_{\varepsilon} are linear, (c+c′)∘=c∘+c′∘(c+c')^{\circ}=c^{\circ}+c'^{\circ} and (λc)∘=λc∘(\lambda c)^{\circ}=\lambda c^{\circ} for c′∈Aεc'\in A_{\varepsilon}, λ∈C\lambda\in\mathbb{C}; and c=c∘+πε(Eε(c))c=c^{\circ}+\pi_{\varepsilon}(E_{\varepsilon}(c)) by definition of the centred part (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §centred). (F3) πε(y)∘=πε(y)−πε(y)=0\pi_{\varepsilon}(y)^{\circ}=\pi_{\varepsilon}(y)-\pi_{\varepsilon}(y)=0, in particular I∘=0I^{\circ}=0 as I=πε(I)I=\pi_{\varepsilon}(I); and a∘=a−πε(0)=aa^{\circ}=a-\pi_{\varepsilon}(0)=a for a∈Aε∘a\in A_{\varepsilon}^{\circ}. (F4) (c πε(y))∘=c πε(y)−πε(Eε(c) y)=c πε(y)−πε(Eε(c))πε(y)=c∘πε(y)(c\,\pi_{\varepsilon}(y))^{\circ}=c\,\pi_{\varepsilon}(y)-\pi_{\varepsilon}(E_{\varepsilon}(c)\,y)=c\,\pi_{\varepsilon}(y)-\pi_{\varepsilon}(E_{\varepsilon}(c))\pi_{\varepsilon}(y)=c^{\circ}\pi_{\varepsilon}(y), by (F1). By The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §centred, b∘b^{\circ}, πε(x) a\pi_{\varepsilon}(x)\,a and a πε(x)a\,\pi_{\varepsilon}(x) are centred for b∈Aεb\in A_{\varepsilon}, a∈Aε∘a\in A_{\varepsilon}^{\circ}, x∈Nx\in N, and sums and scalar multiples of centred elements are centred since EεE_{\varepsilon} is linear; this is why every tuple written below is an alternating tuple: each new entry below is a centred part c∘c^{\circ}, a product π(y) a\pi(y)\,a or a π(y)a\,\pi(y) with aa centred, or a sum or scalar multiple of centred elements, and it stands in the position of an entry of the same algebra. We also use three general facts.

(P0) Vanishing on basis vectors. Let WW be a complex vector space and D:F→WD:\mathcal{F}\to W additive with D(c δu)=0D(c\,\delta_{u})=0 for all c∈Cc\in\mathbb{C} and u∈Tu\in\mathcal{T}. Then D=0D=0. Indeed, D(0)=D(0+0)=D(0)+D(0)D(0)=D(0+0)=D(0)+D(0) gives D(0)=0D(0)=0, which settles ξ\xi with empty support, as then ξ=0\xi=0. If supp⁡ξ\operatorname{supp}\xi has n∈Nn\in\mathbb{N} elements and the claim holds for supports with n−1n-1 elements, pick u∈supp⁡ξu\in\operatorname{supp}\xi and let ξ′=ξ+(−ξ(u))δu\xi'=\xi+(-\xi(u))\delta_{u} (operations of The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §space); then ξ′(u)=0\xi'(u)=0 and ξ′(s)=ξ(s)\xi'(s)=\xi(s) for s≠us\neq u, so supp⁡ξ′=supp⁡ξ∖{u}\operatorname{supp}\xi'=\operatorname{supp}\xi\setminus\{u\} has n−1n-1 elements, ξ=ξ′+ξ(u)δu\xi=\xi'+\xi(u)\delta_{u}, and Dξ=Dξ′+D(ξ(u)δu)=0D\xi=D\xi'+D(\xi(u)\delta_{u})=0. In particular two linear maps F→W\mathcal{F}\to W that agree on every δu\delta_{u} are equal (apply (P0) to their difference).

(P1) The canonical map. By The Amalgamated Free Product Space of Two Noncommutative Laws over a Common Marginal, Its Vacuum Vector and Vacuum State §space, H\mathcal{H} is a complex Hilbert space whose inner product is the pairing of the completion and JJ is its canonical map, so by The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §isometry JJ is complex-linear and ⟨Jξ,Jη⟩H=h(ξ,η)\langle J\xi,J\eta\rangle_{\mathcal{H}}=h(\xi,\eta) for ξ,η∈F\xi,\eta\in\mathcal{F}. Hence ∥Jξ∥H2=h(ξ,ξ)\lVert J\xi\rVert_{\mathcal{H}}^{2}=h(\xi,\xi) by definition of the induced norm, and Jζ=0J\zeta=0 if h(ζ,ζ)=0h(\zeta,\zeta)=0, by definiteness (claim 4 of Elementary Properties of a Complex Inner Product).

(P2) Comparison. If ξ,η∈F\xi,\eta\in\mathcal{F} satisfy h(δσ,ξ)=h(δσ,η)h(\delta_{\sigma},\xi)=h(\delta_{\sigma},\eta) for every σ∈T\sigma\in\mathcal{T}, then Jξ=JηJ\xi=J\eta. Indeed, let ζ=ξ+(−1)η\zeta=\xi+(-1)\eta; by the linearity of hh in its second argument (The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §form), h(δσ,ζ)=0h(\delta_{\sigma},\zeta)=0 for every σ\sigma. The map D(χ)=h(χ,ζ)D(\chi)=h(\chi,\zeta) is additive and satisfies D(c χ)=c‾ D(χ)D(c\,\chi)=\overline{c}\,D(\chi), because h(χ,ζ)=h(ζ,χ)‾h(\chi,\zeta)=\overline{h(\zeta,\chi)} and h(ζ,⋅)h(\zeta,\cdot) is linear (The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §form); so D(c δσ)=0D(c\,\delta_{\sigma})=0 for all c,σc,\sigma, and D=0D=0 by (P0). Thus h(ζ,ζ)=0h(\zeta,\zeta)=0, Jζ=0J\zeta=0 by (P1), and Jξ=JηJ\xi=J\eta since JJ is linear. We shall use (P2) with ξ,η\xi,\eta sums of vectors δτ\delta_{\tau}, computing h(δσ,δτ)=h0(σ,τ)h(\delta_{\sigma},\delta_{\tau})=h_{0}(\sigma,\tau) by The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §form and expanding by linearity in the second argument. Recall from The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §form that h0(σ,(k,t))=0h_{0}(\sigma,(k,t))=0 unless σ=(k,s)\sigma=(k,s) with ss of the same length and type as tt, and then h0(σ,(k,t))=τμ(Xk(s,t))h_{0}(\sigma,(k,t))=\tau_{\mu}(X_{k}(s,t)); τμ\tau_{\mu} is linear by The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots §trace.

Claim 1 (Multilinearity). For x,y∈Nx,y\in N, c∈Cc\in\mathbb{C} and σ∈T\sigma\in\mathcal{T}: if σ=(0,z)\sigma=(0,z) then h0(σ,(0,x+y))=τμ(z∗x)+τμ(z∗y)h_{0}(\sigma,(0,x+y))=\tau_{\mu}(z^{*}x)+\tau_{\mu}(z^{*}y) and h0(σ,(0,cx))=c τμ(z∗x)h_{0}(\sigma,(0,cx))=c\,\tau_{\mu}(z^{*}x) by linearity of τμ\tau_{\mu}, and for every other σ\sigma all these pairings vanish. So h(δσ,δx+yN)=h(δσ,δxN+δyN)h(\delta_{\sigma},\delta^{N}_{x+y})=h(\delta_{\sigma},\delta^{N}_{x}+\delta^{N}_{y}) and h(δσ,δcxN)=h(δσ,c δxN)h(\delta_{\sigma},\delta^{N}_{cx})=h(\delta_{\sigma},c\,\delta^{N}_{x}) for every σ\sigma, and (P2) with the linearity of JJ gives ΞN(x+y)=ΞN(x)+ΞN(y)\Xi_{N}(x+y)=\Xi_{N}(x)+\Xi_{N}(y) and ΞN(cx)=c ΞN(x)\Xi_{N}(cx)=c\,\Xi_{N}(x).

For the tuple vectors, let t=(a1,…,ak)t=(a_{1},\dots,a_{k}), let t′t' be tt with aja_{j} replaced by aj′a_{j}', t′′t'' the same with aj+aj′a_{j}+a_{j}', and tct_{c} the same with c ajc\,a_{j}. Let s=(d1,…,dk)s=(d_{1},\dots,d_{k}) have the same type. We show by induction on i∈[k]i\in[k] that Xi(s,t′′)=Xi(s,t)=Xi(s,t′)X_{i}(s,t'')=X_{i}(s,t)=X_{i}(s,t') and Xi(s,tc)=Xi(s,t)X_{i}(s,t_{c})=X_{i}(s,t) for i<ji<j, and Xi(s,t′′)=Xi(s,t)+Xi(s,t′)X_{i}(s,t'')=X_{i}(s,t)+X_{i}(s,t') and Xi(s,tc)=c Xi(s,t)X_{i}(s,t_{c})=c\,X_{i}(s,t) for i≥ji\ge j (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §nested). For i<ji<j the recursion for XiX_{i} involves only entries with index at most ii, which coincide in the four tuples, and previous terms which coincide by induction. For i=ji=j the entry aj+aj′a_{j}+a_{j}' (resp. c ajc\,a_{j}) enters linearly: Xj(s,t′′)=Eej(dj∗P(aj+aj′))=Eej(dj∗Paj)+Eej(dj∗Paj′)X_{j}(s,t'')=E_{e_{j}}(d_{j}^{*}P(a_{j}+a_{j}'))=E_{e_{j}}(d_{j}^{*}Pa_{j})+E_{e_{j}}(d_{j}^{*}Pa_{j}'), where P=IP=I if j=1j=1 and P=πej(Xj−1(s,t))P=\pi_{e_{j}}(X_{j-1}(s,t)) otherwise, which is common to the tuples; likewise for tct_{c}. For i>ji>j, Xi(s,t′′)=Eei(di∗πei(Xi−1(s,t)+Xi−1(s,t′))ai)=Xi(s,t)+Xi(s,t′)X_{i}(s,t'')=E_{e_{i}}(d_{i}^{*}\pi_{e_{i}}(X_{i-1}(s,t)+X_{i-1}(s,t'))a_{i})=X_{i}(s,t)+X_{i}(s,t') by linearity of πei\pi_{e_{i}} and EeiE_{e_{i}}, and likewise Xi(s,tc)=c Xi(s,t)X_{i}(s,t_{c})=c\,X_{i}(s,t). With i=ki=k and linearity of τμ\tau_{\mu}, h0(σ,(k,t′′))=h0(σ,(k,t))+h0(σ,(k,t′))h_{0}(\sigma,(k,t''))=h_{0}(\sigma,(k,t))+h_{0}(\sigma,(k,t')) and h0(σ,(k,tc))=c h0(σ,(k,t))h_{0}(\sigma,(k,t_{c}))=c\,h_{0}(\sigma,(k,t)) for σ=(k,s)\sigma=(k,s) with ss of the type of tt, and all these pairings vanish for every other σ\sigma, since t,t′,t′′,tct,t',t'',t_{c} share length and type. Hence h(δσ,δt′′)=h(δσ,δt+δt′)h(\delta_{\sigma},\delta_{t''})=h(\delta_{\sigma},\delta_{t}+\delta_{t'}) and h(δσ,δtc)=h(δσ,c δt)h(\delta_{\sigma},\delta_{t_{c}})=h(\delta_{\sigma},c\,\delta_{t}) for all σ\sigma, and (P2) and linearity of JJ give the two identities. Finally, if aj=0a_{j}=0 then aj=0⋅aja_{j}=0\cdot a_{j}, so Ξ(a1,…,ak)=0⋅Ξ(a1,…,ak)=0\Xi(a_{1},\dots,a_{k})=0\cdot\Xi(a_{1},\dots,a_{k})=0; in the same way ΞN(0)=0\Xi_{N}(0)=0.

Claim 2 (Balance over NN). Let t=(a1,…,ak)t=(a_{1},\dots,a_{k}), j<kj<k, x∈Nx\in N, let t′t' be tt with aja_{j} replaced by ajπej(x)a_{j}\pi_{e_{j}}(x) and t′′t'' be tt with aj+1a_{j+1} replaced by πej+1(x)aj+1\pi_{e_{j+1}}(x)a_{j+1}; both are alternating of the type of tt. Let s=(d1,…,dk)s=(d_{1},\dots,d_{k}) have this type. For i<ji<j, Xi(s,t′)=Xi(s,t′′)=Xi(s,t)X_{i}(s,t')=X_{i}(s,t'')=X_{i}(s,t) as in Claim 1. With PP as in Claim 1, (F1) gives Xj(s,t′)=Eej(dj∗Pajπej(x))=Xj(s,t) xX_{j}(s,t')=E_{e_{j}}(d_{j}^{*}Pa_{j}\pi_{e_{j}}(x))=X_{j}(s,t)\,x, while Xj(s,t′′)=Xj(s,t)X_{j}(s,t'')=X_{j}(s,t). Then, πej+1\pi_{e_{j+1}} being multiplicative,

Xj+1(s,t′)=Eej+1(dj+1∗πej+1(Xj(s,t) x) aj+1)=Eej+1(dj+1∗πej+1(Xj(s,t)) πej+1(x)aj+1)=Xj+1(s,t′′),X_{j+1}(s,t')=E_{e_{j+1}}\bigl(d_{j+1}^{*}\pi_{e_{j+1}}(X_{j}(s,t)\,x)\,a_{j+1}\bigr)=E_{e_{j+1}}\bigl(d_{j+1}^{*}\pi_{e_{j+1}}(X_{j}(s,t))\,\pi_{e_{j+1}}(x)a_{j+1}\bigr)=X_{j+1}(s,t''),

and for i>j+1i>j+1 the recursions for t′t' and t′′t'' use the same entries and, by induction, equal previous terms, so Xk(s,t′)=Xk(s,t′′)X_{k}(s,t')=X_{k}(s,t''). Hence h0(σ,(k,t′))=h0(σ,(k,t′′))h_{0}(\sigma,(k,t'))=h_{0}(\sigma,(k,t'')) for all σ∈T\sigma\in\mathcal{T} (both vanish unless σ=(k,s)\sigma=(k,s) as above), and (P2) gives Ξ(t′)=Ξ(t′′)\Xi(t')=\Xi(t'').

Claim 3 (Relations). For each identity, both sides are linear maps F→H\mathcal{F}\to\mathcal{H} of ξ\xi, as composites, sums and scalar multiples of the linear maps JJ (P1) and ℓε(⋅)\ell_{\varepsilon}(\cdot) (The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §actions); so by (P0) it suffices to take ξ=δu\xi=\delta_{u}, u∈Tu\in\mathcal{T}. By The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §actions, ℓε(b)δu=ρε,b(u)\ell_{\varepsilon}(b)\delta_{u}=\rho_{\varepsilon,b}(u), and Jρε,b(u)J\rho_{\varepsilon,b}(u) is the sum of the two vectors Ξ(⋅)\Xi(\cdot) or ΞN(⋅)\Xi_{N}(\cdot) (The Amalgamated Free Product Space of Two Noncommutative Laws over a Common Marginal, Its Vacuum Vector and Vacuum State §vectors) of the two labels in The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §actions, as JJ is linear. We write π=πε\pi=\pi_{\varepsilon}, E=EεE=E_{\varepsilon}, ρb=ρε,b\rho_{b}=\rho_{\varepsilon,b}, and let t=(a1,…,ak)t=(a_{1},\dots,a_{k}) denote a tuple of type (e1,…,ek)(e_{1},\dots,e_{k}).

Linearity in bb. In each case (a), (b), (c) of The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §actions the two labels of ρb(u)\rho_{b}(u) depend on bb through one entry each, namely (bπ(x))∘(b\pi(x))^{\circ} and E(bπ(x))E(b\pi(x)); b∘b^{\circ} and πe1(E(b))a1\pi_{e_{1}}(E(b))a_{1}; (ba1)∘(ba_{1})^{\circ} and πe2(E(ba1))a2\pi_{e_{2}}(E(ba_{1}))a_{2} (or E(ba1)E(ba_{1}) if k=1k=1). By (F2) and the linearity of EE and πe1\pi_{e_{1}}, πe2\pi_{e_{2}}, each of these entries for b+b′b+b' (resp. cbcb) is the sum of the entries for bb and b′b' (resp. cc times the entry for bb). Claim 1 applied in that entry, and rearranging the four resulting vectors, gives Jρb+b′(u)=Jρb(u)+Jρb′(u)J\rho_{b+b'}(u)=J\rho_{b}(u)+J\rho_{b'}(u) and Jρcb(u)=c Jρb(u)J\rho_{cb}(u)=c\,J\rho_{b}(u).

Unit. For u=(0,x)u=(0,x): Iπ(x)=π(x)I\pi(x)=\pi(x), π(x)∘=0\pi(x)^{\circ}=0 (F3) and E(π(x))=xE(\pi(x))=x, so JρI(u)=Ξ((ε,0))+ΞN(x)=ΞN(x)=JδuJ\rho_{I}(u)=\Xi((\varepsilon,0))+\Xi_{N}(x)=\Xi_{N}(x)=J\delta_{u} by Claim 1, where Ξ((ε,0))\Xi((\varepsilon,0)) denotes the vector of the one-entry tuple ((ε,0))((\varepsilon,0)). For u=(k,t)u=(k,t) with e1=εˉe_{1}=\bar{\varepsilon}: I∘=0I^{\circ}=0 (F3) and πe1(E(I))a1=πe1(I)a1=a1\pi_{e_{1}}(E(I))a_{1}=\pi_{e_{1}}(I)a_{1}=a_{1}, so JρI(u)=Ξ(0,a1,…,ak)+Ξ(t)=Ξ(t)J\rho_{I}(u)=\Xi(0,a_{1},\dots,a_{k})+\Xi(t)=\Xi(t) by Claim 1. For u=(k,t)u=(k,t) with e1=εe_{1}=\varepsilon: (Ia1)∘=a1(Ia_{1})^{\circ}=a_{1} (F3) and E(a1)=0E(a_{1})=0, so JρI(u)J\rho_{I}(u) is Ξ(t)+Ξ(πe2(0)a2,a3,…,ak)=Ξ(t)+Ξ(0,a3,…,ak)=Ξ(t)\Xi(t)+\Xi(\pi_{e_{2}}(0)a_{2},a_{3},\dots,a_{k})=\Xi(t)+\Xi(0,a_{3},\dots,a_{k})=\Xi(t) if k≥2k\ge2 and Ξ(t)+ΞN(0)=Ξ(t)\Xi(t)+\Xi_{N}(0)=\Xi(t) if k=1k=1, by Claim 1.

Amalgamation. Let x∈Nx\in N and bε=πε(x)b_{\varepsilon}=\pi_{\varepsilon}(x), so bε∘=0b_{\varepsilon}^{\circ}=0 by (F3) and Eε(bε)=xE_{\varepsilon}(b_{\varepsilon})=x by Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §expectation. For u=(0,y)u=(0,y) and either ε\varepsilon: bεπε(y)=πε(xy)b_{\varepsilon}\pi_{\varepsilon}(y)=\pi_{\varepsilon}(xy), so Jρε,bε(u)=Ξ((ε,0))+ΞN(xy)=ΞN(xy)J\rho_{\varepsilon,b_{\varepsilon}}(u)=\Xi((\varepsilon,0))+\Xi_{N}(xy)=\Xi_{N}(xy) by (F3) and Claim 1; the two sides agree. For u=(k,t)u=(k,t) with e1=εe_{1}=\varepsilon (so e2=εˉe_{2}=\bar{\varepsilon} if k≥2k\ge2): the action of bεb_{\varepsilon} is case (c); πε(x)a1\pi_{\varepsilon}(x)a_{1} is centred, so (πε(x)a1)∘=πε(x)a1(\pi_{\varepsilon}(x)a_{1})^{\circ}=\pi_{\varepsilon}(x)a_{1} (F3) and Eε(πε(x)a1)=x Eε(a1)=0E_{\varepsilon}(\pi_{\varepsilon}(x)a_{1})=x\,E_{\varepsilon}(a_{1})=0 (F1); by Claim 1, Jρε,bε(u)=Ξ(πε(x)a1,a2,…,ak)+Ξ(0,a3,…,ak)J\rho_{\varepsilon,b_{\varepsilon}}(u)=\Xi(\pi_{\varepsilon}(x)a_{1},a_{2},\dots,a_{k})+\Xi(0,a_{3},\dots,a_{k}) if k≥2k\ge2, and Ξ(πε(x)a1)+ΞN(0)\Xi(\pi_{\varepsilon}(x)a_{1})+\Xi_{N}(0) if k=1k=1, which in both cases equals Ξ(πε(x)a1,a2,…,ak)\Xi(\pi_{\varepsilon}(x)a_{1},a_{2},\dots,a_{k}). The action of bεˉb_{\bar{\varepsilon}} is case (b), with εˉ\bar{\varepsilon} in the role of ε\varepsilon: Jρεˉ,bεˉ(u)=Ξ(0,a1,…,ak)+Ξ(πε(x)a1,a2,…,ak)J\rho_{\bar{\varepsilon},b_{\bar{\varepsilon}}}(u)=\Xi(0,a_{1},\dots,a_{k})+\Xi(\pi_{\varepsilon}(x)a_{1},a_{2},\dots,a_{k}), the same vector by Claim 1. Thus Jℓ1(π1(x))δu=Jℓ2(π2(x))δuJ\ell_{1}(\pi_{1}(x))\delta_{u}=J\ell_{2}(\pi_{2}(x))\delta_{u} for every uu.

Multiplicativity. Let b,b′∈Aεb,b'\in A_{\varepsilon} and write ρb′(u)=δv+δw\rho_{b'}(u)=\delta_{v}+\delta_{w} as in The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §actions; by linearity of ℓε(b)\ell_{\varepsilon}(b) and The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §actions, Jℓε(b)ℓε(b′)δu=Jρb(v)+Jρb(w)J\ell_{\varepsilon}(b)\ell_{\varepsilon}(b')\delta_{u}=J\rho_{b}(v)+J\rho_{b}(w), which we compare with Jρbb′(u)J\rho_{bb'}(u).

Case u=(0,x)u=(0,x), or u=(1,t)u=(1,t) with e1=εe_{1}=\varepsilon. Let g=π(x)g=\pi(x), resp. g=a1g=a_{1}, and f=(b′g)∘f=(b'g)^{\circ}, y=E(b′g)y=E(b'g); then vv is the one-entry tuple ((ε,f))((\varepsilon,f)) and w=(0,y)w=(0,y), and b′g=f+π(y)b'g=f+\pi(y) (F2). By cases (c) with k=1k=1 and (a), Jρb(v)+Jρb(w)=Ξ((bf)∘)+ΞN(E(bf))+Ξ((bπ(y))∘)+ΞN(E(bπ(y)))J\rho_{b}(v)+J\rho_{b}(w)=\Xi((bf)^{\circ})+\Xi_{N}(E(bf))+\Xi((b\pi(y))^{\circ})+\Xi_{N}(E(b\pi(y))), while Jρbb′(u)=Ξ((bb′g)∘)+ΞN(E(bb′g))J\rho_{bb'}(u)=\Xi((bb'g)^{\circ})+\Xi_{N}(E(bb'g)) in both cases. Since bb′g=bf+bπ(y)bb'g=bf+b\pi(y), (F2) and linearity of EE give (bb′g)∘=(bf)∘+(bπ(y))∘(bb'g)^{\circ}=(bf)^{\circ}+(b\pi(y))^{\circ} and E(bb′g)=E(bf)+E(bπ(y))E(bb'g)=E(bf)+E(b\pi(y)), and Claim 1 gives equality.

Case u=(k,t)u=(k,t) with e1=εˉe_{1}=\bar{\varepsilon}. Here v=(b′∘,a1,…,ak)v=(b'^{\circ},a_{1},\dots,a_{k}), of type (ε,e1,…,ek)(\varepsilon,e_{1},\dots,e_{k}) and length k+1≥2k+1\ge2, and w=(πe1(E(b′))a1,a2,…,ak)w=(\pi_{e_{1}}(E(b'))a_{1},a_{2},\dots,a_{k}). Case (c) for vv and case (b) for ww give

Jρb(v)+Jρb(w)=Ξ((bb′∘)∘,a1,…,ak)+Ξ(πe1(E(bb′∘))a1,a2,…,ak)+Ξ(b∘,πe1(E(b′))a1,a2,…,ak)+Ξ(πe1(E(b))πe1(E(b′))a1,a2,…,ak),J\rho_{b}(v)+J\rho_{b}(w)=\Xi((bb'^{\circ})^{\circ},a_{1},\dots,a_{k})+\Xi(\pi_{e_{1}}(E(bb'^{\circ}))a_{1},a_{2},\dots,a_{k})+\Xi(b^{\circ},\pi_{e_{1}}(E(b'))a_{1},a_{2},\dots,a_{k})+\Xi(\pi_{e_{1}}(E(b))\pi_{e_{1}}(E(b'))a_{1},a_{2},\dots,a_{k}),

and Jρbb′(u)=Ξ((bb′)∘,a1,…,ak)+Ξ(πe1(E(bb′))a1,a2,…,ak)J\rho_{bb'}(u)=\Xi((bb')^{\circ},a_{1},\dots,a_{k})+\Xi(\pi_{e_{1}}(E(bb'))a_{1},a_{2},\dots,a_{k}). By (F2), bb′=bb′∘+b π(E(b′))bb'=bb'^{\circ}+b\,\pi(E(b')), so by (F2), (F4) and (F1), (bb′)∘=(bb′∘)∘+b∘π(E(b′))(bb')^{\circ}=(bb'^{\circ})^{\circ}+b^{\circ}\pi(E(b')) and E(bb′)=E(bb′∘)+E(b)E(b′)E(bb')=E(bb'^{\circ})+E(b)E(b'), whence πe1(E(bb′))a1=πe1(E(bb′∘))a1+πe1(E(b))πe1(E(b′))a1\pi_{e_{1}}(E(bb'))a_{1}=\pi_{e_{1}}(E(bb'^{\circ}))a_{1}+\pi_{e_{1}}(E(b))\pi_{e_{1}}(E(b'))a_{1}. Claim 1 in the first entry splits the first vector of Jρbb′(u)J\rho_{bb'}(u) into Ξ((bb′∘)∘,a1,…,ak)+Ξ(b∘π(E(b′)),a1,…,ak)\Xi((bb'^{\circ})^{\circ},a_{1},\dots,a_{k})+\Xi(b^{\circ}\pi(E(b')),a_{1},\dots,a_{k}), and Claim 2 (with j=1<k+1j=1<k+1) turns the latter into Ξ(b∘,πe1(E(b′))a1,a2,…,ak)\Xi(b^{\circ},\pi_{e_{1}}(E(b'))a_{1},a_{2},\dots,a_{k}); Claim 1 in the first entry splits the second vector into the second and fourth vectors above. So the two sides agree.

Case u=(k,t)u=(k,t) with e1=εe_{1}=\varepsilon and k≥2k\ge2. Let f=(b′a1)∘f=(b'a_{1})^{\circ} and y=E(b′a1)y=E(b'a_{1}), so b′a1=f+π(y)b'a_{1}=f+\pi(y) (F2). Here v=(f,a2,…,ak)v=(f,a_{2},\dots,a_{k}), of length k≥2k\ge2 starting with ε\varepsilon, and w=(πe2(y)a2,a3,…,ak)w=(\pi_{e_{2}}(y)a_{2},a_{3},\dots,a_{k}), of length k−1k-1 starting with e2=εˉe_{2}=\bar{\varepsilon}. Case (c) for vv and case (b) for ww give

Jρb(v)+Jρb(w)=Ξ((bf)∘,a2,…,ak)+Ξ(πe2(E(bf))a2,a3,…,ak)+Ξ(b∘,πe2(y)a2,a3,…,ak)+Ξ(πe2(E(b))πe2(y)a2,a3,…,ak),J\rho_{b}(v)+J\rho_{b}(w)=\Xi((bf)^{\circ},a_{2},\dots,a_{k})+\Xi(\pi_{e_{2}}(E(bf))a_{2},a_{3},\dots,a_{k})+\Xi(b^{\circ},\pi_{e_{2}}(y)a_{2},a_{3},\dots,a_{k})+\Xi(\pi_{e_{2}}(E(b))\pi_{e_{2}}(y)a_{2},a_{3},\dots,a_{k}),

and Jρbb′(u)=Ξ((bb′a1)∘,a2,…,ak)+Ξ(πe2(E(bb′a1))a2,a3,…,ak)J\rho_{bb'}(u)=\Xi((bb'a_{1})^{\circ},a_{2},\dots,a_{k})+\Xi(\pi_{e_{2}}(E(bb'a_{1}))a_{2},a_{3},\dots,a_{k}). As bb′a1=bf+b π(y)bb'a_{1}=bf+b\,\pi(y), (F2), (F4) and (F1) give (bb′a1)∘=(bf)∘+b∘π(y)(bb'a_{1})^{\circ}=(bf)^{\circ}+b^{\circ}\pi(y) and E(bb′a1)=E(bf)+E(b) yE(bb'a_{1})=E(bf)+E(b)\,y. Exactly as in the previous case, Claim 1 in the first entry and Claim 2 (with j=1<kj=1<k) identify the two sides.

Claim 4 (Bound). Let b∈Aεb\in A_{\varepsilon} and β=∥b∥op\beta=\lVert b\rVert_{\mathrm{op}}. Since AεA_{\varepsilon} is the tracial algebra of γε∈Σmε\gamma_{\varepsilon}\in\Sigma_{m_{\varepsilon}} (Two Noncommutative Laws with a Common Marginal: Standing Notation for Their Amalgamated Free Product §data, Two Noncommutative Laws with a Common Marginal: Standing Notation for Their Amalgamated Free Product §algebras), The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots §positivity gives T=β2I−b∗b≥0T=\beta^{2}I-b^{*}b\ge0, where T∈AεT\in A_{\varepsilon} by The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots §star-algebra, and then q∈Aεq\in A_{\varepsilon} with q≥0q\ge0 and qq=Tqq=T. As q≥0q\ge0, qq is self-adjoint (Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation §maps), hence an adjoint of itself (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus), so q∗=qq^{*}=q by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique and q∗q=Tq^{*}q=T. For d∈Aεd\in A_{\varepsilon} and ξ∈F\xi\in\mathcal{F}, (P1), the adjoint relation of The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions §actions and multiplicativity in Claim 3 give

∥Jℓε(d)ξ∥H2=h(ℓε(d)ξ,ℓε(d)ξ)=h(ξ,ℓε(d∗)ℓε(d)ξ)=⟨Jξ,Jℓε(d∗)ℓε(d)ξ⟩H=⟨Jξ,Jℓε(d∗d)ξ⟩H.\lVert J\ell_{\varepsilon}(d)\xi\rVert_{\mathcal{H}}^{2}=h(\ell_{\varepsilon}(d)\xi,\ell_{\varepsilon}(d)\xi)=h(\xi,\ell_{\varepsilon}(d^{*})\ell_{\varepsilon}(d)\xi)=\langle J\xi,J\ell_{\varepsilon}(d^{*})\ell_{\varepsilon}(d)\xi\rangle_{\mathcal{H}}=\langle J\xi,J\ell_{\varepsilon}(d^{*}d)\xi\rangle_{\mathcal{H}}.

Taking d=qd=q and using linearity in bb and the unit relation of Claim 3, Jℓε(T)ξ=β2Jξ−Jℓε(b∗b)ξJ\ell_{\varepsilon}(T)\xi=\beta^{2}J\xi-J\ell_{\varepsilon}(b^{*}b)\xi, so, taking also d=bd=b,

0≤∥Jℓε(q)ξ∥H2=β2⟨Jξ,Jξ⟩H−⟨Jξ,Jℓε(b∗b)ξ⟩H=β2∥Jξ∥H2−∥Jℓε(b)ξ∥H2.0\le\lVert J\ell_{\varepsilon}(q)\xi\rVert_{\mathcal{H}}^{2}=\beta^{2}\langle J\xi,J\xi\rangle_{\mathcal{H}}-\langle J\xi,J\ell_{\varepsilon}(b^{*}b)\xi\rangle_{\mathcal{H}}=\beta^{2}\lVert J\xi\rVert_{\mathcal{H}}^{2}-\lVert J\ell_{\varepsilon}(b)\xi\rVert_{\mathcal{H}}^{2}.

Thus ∥Jℓε(b)ξ∥H2≤(β∥Jξ∥H)2\lVert J\ell_{\varepsilon}(b)\xi\rVert_{\mathcal{H}}^{2}\le(\beta\lVert J\xi\rVert_{\mathcal{H}})^{2}; both ∥Jℓε(b)ξ∥H\lVert J\ell_{\varepsilon}(b)\xi\rVert_{\mathcal{H}} and β∥Jξ∥H\beta\lVert J\xi\rVert_{\mathcal{H}} are nonnegative reals (β≥0\beta\ge0 as β\beta is a bound, Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound and Bounded Linear Maps between Complex Normed Spaces and the Operator Norm §bounded), so claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives ∥Jℓε(b)ξ∥H≤β∥Jξ∥H\lVert J\ell_{\varepsilon}(b)\xi\rVert_{\mathcal{H}}\le\beta\lVert J\xi\rVert_{\mathcal{H}}.

Claim 5 (Actions). Let b∈Aεb\in A_{\varepsilon}, β=∥b∥op\beta=\lVert b\rVert_{\mathrm{op}}, and Tb:F→HT_{b}:\mathcal{F}\to\mathcal{H}, Tbξ=Jℓε(b)ξT_{b}\xi=J\ell_{\varepsilon}(b)\xi. Then TbT_{b} is complex-linear, being a composite of linear maps, and ∥Tbξ∥H2≤β2∥Jξ∥H2=β2h(ξ,ξ)\lVert T_{b}\xi\rVert_{\mathcal{H}}^{2}\le\beta^{2}\lVert J\xi\rVert_{\mathcal{H}}^{2}=\beta^{2}h(\xi,\xi) by Claim 4 and (P1). By The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §extension-linear with V=FV=\mathcal{F}, the form hh, K=HK=\mathcal{H} and C=βC=\beta (the completion being H\mathcal{H} and Jh=JJ_{h}=J by The Amalgamated Free Product Space of Two Noncommutative Laws over a Common Marginal, Its Vacuum Vector and Vacuum State §space), there is exactly one continuous map Λε(b):H→H\Lambda_{\varepsilon}(b):\mathcal{H}\to\mathcal{H} with Λε(b)Jξ=Jℓε(b)ξ\Lambda_{\varepsilon}(b)J\xi=J\ell_{\varepsilon}(b)\xi for every ξ∈F\xi\in\mathcal{F}, and it belongs to L(H)\mathcal{L}(\mathcal{H}) with bound β\beta; hence ∥Λε(b)∥op≤β\lVert\Lambda_{\varepsilon}(b)\rVert_{\mathrm{op}}\le\beta by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound. For uniqueness within L(H)\mathcal{L}(\mathcal{H}), let S∈L(H)S\in\mathcal{L}(\mathcal{H}) satisfy SJξ=Jℓε(b)ξSJ\xi=J\ell_{\varepsilon}(b)\xi for every ξ\xi. For w,w′∈Hw,w'\in\mathcal{H}, linearity of SS and the fact that ∥S∥op\lVert S\rVert_{\mathrm{op}} is a bound for SS (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound) give ∥Sw−Sw′∥H=∥S(w−w′)∥H≤∥S∥op∥w−w′∥H\lVert Sw-Sw'\rVert_{\mathcal{H}}=\lVert S(w-w')\rVert_{\mathcal{H}}\le\lVert S\rVert_{\mathrm{op}}\lVert w-w'\rVert_{\mathcal{H}}. The metric of H\mathcal{H} is (w,w′)↦∥w−w′∥H(w,w')\mapsto\lVert w-w'\rVert_{\mathcal{H}} (Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation §spaces, claim 3 of The Induced Norm is a Norm, and Induces a Metric), so SS is Lipschitz with constant ∥S∥op\lVert S\rVert_{\mathrm{op}} and therefore continuous by A Lipschitz Map is Uniformly Continuous. By the uniqueness in The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §extension-linear, S=Λε(b)S=\Lambda_{\varepsilon}(b).

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