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Proof of The Formal Amalgamated Free Product: the Free Vector Space, Positivity of the Nested-Expectation Form, and Linearity and Formal Adjoints of the Actions

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· 25,035 chars · 23 deps · depth 23 Reason: G4: proof of positivity of the nested-expectation form and formal adjoints.

Pointwise checks give the vector space; positivity of the Gram operators follows by induction on length using square roots whose blocks lie in the marginal algebra; the formal adjoint identity is checked on basis vectors in six label cases.

Proof

Conventions. For ε∈{1,2}\varepsilon\in\{1,2\} let Vε∈L(Hμ,Hγε)V_{\varepsilon}\in\mathcal{L}(\mathcal{H}_{\mu},\mathcal{H}_{\gamma_{\varepsilon}}) be the operator of Marginals of a Noncommutative Law: the Isometry of GNS Spaces, the Trace-Preserving Embedding of Tracial Algebras and the Conditional Expectation §isometry for γ=γε\gamma=\gamma_{\varepsilon} and a=aεa=a^{\varepsilon} (an operator, not an inner product space); by Two Noncommutative Laws with a Common Marginal: Standing Notation for Their Amalgamated Free Product §embeddings, πε\pi_{\varepsilon} and EεE_{\varepsilon} are the embedding and the expectation of that lemma for the same data. By 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, πε\pi_{\varepsilon} and EεE_{\varepsilon} are linear and, for S,T∈NS,T\in N, c∈Aεc\in A_{\varepsilon} and ζ,ζ′∈Hμ\zeta,\zeta'\in\mathcal{H}_{\mu},

πε(I)=I,πε(ST)=πε(S)πε(T),πε(T∗)=πε(T)∗,Eε(c∗)=Eε(c)∗,Eε(πε(S) c πε(T))=S Eε(c) T,⟨ζ,Eε(c)ζ′⟩=⟨Vεζ,cVεζ′⟩;\pi_{\varepsilon}(I)=I,\quad\pi_{\varepsilon}(ST)=\pi_{\varepsilon}(S)\pi_{\varepsilon}(T),\quad\pi_{\varepsilon}(T^{*})=\pi_{\varepsilon}(T)^{*},\quad E_{\varepsilon}(c^{*})=E_{\varepsilon}(c)^{*},\quad E_{\varepsilon}(\pi_{\varepsilon}(S)\,c\,\pi_{\varepsilon}(T))=S\,E_{\varepsilon}(c)\,T,\quad\langle\zeta,E_{\varepsilon}(c)\zeta'\rangle=\langle V_{\varepsilon}\zeta,cV_{\varepsilon}\zeta'\rangle;

with T=IT=I or S=IS=I this gives Eε(πε(S)c)=S Eε(c)E_{\varepsilon}(\pi_{\varepsilon}(S)c)=S\,E_{\varepsilon}(c) and Eε(c πε(T))=Eε(c) TE_{\varepsilon}(c\,\pi_{\varepsilon}(T))=E_{\varepsilon}(c)\,T. The GNS spaces Hμ\mathcal{H}_{\mu}, Hγε\mathcal{H}_{\gamma_{\varepsilon}} are complex Hilbert spaces (The Complex GNS Space of a Tracial State on Noncommutative Polynomials §gns) and NN, AεA_{\varepsilon} consist of bounded operators on them (The Tracial Algebra of a Noncommutative Law and Its Trace §algebra), so all their elements have adjoints (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint); NN and AεA_{\varepsilon} contain II and are closed under sums, scalar multiples, products and adjoints (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), hence are subspaces of the complex vector spaces of Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations, in which composition distributes over sums and commutes with scalar multiples. The rules (S+T)∗=S∗+T∗(S+T)^{*}=S^{*}+T^{*}, (cT)∗=c‾ T∗(cT)^{*}=\overline{c}\,T^{*}, (ST)∗=T∗S∗(ST)^{*}=T^{*}S^{*} and (T∗)∗=T(T^{*})^{*}=T of 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 (with 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) are used freely.

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 §space, an alternating tuple tt of length kk also stands for the label (k,t)(k,t); the labels (0,x)(0,x), x∈Nx\in N, are called NN-labels. By The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §form:

(Z) h0(u,v)=0h_{0}(u,v)=0 unless u,vu,v are both NN-labels or are tuples of the same length and the same type; in particular h0(u,v)=0h_{0}(u,v)=0 if u,vu,v are tuples whose types have different first entries.

Fix the label o=(0,I)o=(0,I) and, for ξ∈F\xi\in\mathcal{F}, put Fξ=supp⁡ξ∪{o}F_{\xi}=\operatorname{supp}\xi\cup\{o\}, a nonempty finite set by claim 1 of Peeling an Element off a Finite Set, and Unions of Finite Sets. A sum over a nonempty finite index set is a finite sum along one bijection from an initial segment (Sum over a Finite Index Set), so claims 2 and 3 of Properties of Finite Sums give

(S) ∑x∈F(f(x)+g(x))=∑x∈Ff(x)+∑x∈Fg(x)\sum_{x\in F}(f(x)+g(x))=\sum_{x\in F}f(x)+\sum_{x\in F}g(x) and ∑x∈Fc f(x)=c∑x∈Ff(x)\sum_{x\in F}c\,f(x)=c\sum_{x\in F}f(x) for maps f,g:F→Cf,g:F\to\mathbb{C} and c∈Cc\in\mathbb{C}.

(C) Centred parts. Let c,d∈Aεc,d\in A_{\varepsilon}. 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, (c∘)∗=c∗−πε(Eε(c))∗=c∗−πε(Eε(c)∗)(c^{\circ})^{*}=c^{*}-\pi_{\varepsilon}(E_{\varepsilon}(c))^{*}=c^{*}-\pi_{\varepsilon}(E_{\varepsilon}(c)^{*}), so by the rules above

Eε((c∘)∗d)=Eε(c∗d)−Eε(c)∗Eε(d)=Eε(c∗d)−Eε(c∗πε(Eε(d)))=Eε(c∗d∘).E_{\varepsilon}((c^{\circ})^{*}d)=E_{\varepsilon}(c^{*}d)-E_{\varepsilon}(c)^{*}E_{\varepsilon}(d)=E_{\varepsilon}(c^{*}d)-E_{\varepsilon}(c^{*}\pi_{\varepsilon}(E_{\varepsilon}(d)))=E_{\varepsilon}(c^{*}d^{\circ}).

In particular, if c∈Aε∘c\in A_{\varepsilon}^{\circ} or d∈Aε∘d\in A_{\varepsilon}^{\circ}, then Eε((c∘)∗d)=Eε(c∗d∘)=Eε(c∗d)E_{\varepsilon}((c^{\circ})^{*}d)=E_{\varepsilon}(c^{*}d^{\circ})=E_{\varepsilon}(c^{*}d), as Eε(c)∗Eε(d)=0E_{\varepsilon}(c)^{*}E_{\varepsilon}(d)=0.

(X) Comparison of layers. Let s=(a1,…,ak)s=(a_{1},\dots,a_{k}), t=(b1,…,bk)t=(b_{1},\dots,b_{k}) be alternating tuples of length kk and common type (e1,…,ek)(e_{1},\dots,e_{k}), let s′=(a1′,…,ak′′)s'=(a'_{1},\dots,a'_{k'}), t′=(b1′,…,bk′′)t'=(b'_{1},\dots,b'_{k'}) be alternating tuples of length k′k' and common type (e1′,…,ek′′)(e'_{1},\dots,e'_{k'}), and let d∈{0,1}d\in\{0,1\} with k+d≤k′k+d\le k'. Suppose X1(s,t)=X1+d(s′,t′)X_{1}(s,t)=X_{1+d}(s',t') and (ej,aj,bj)=(ej+d′,aj+d′,bj+d′)(e_{j},a_{j},b_{j})=(e'_{j+d},a'_{j+d},b'_{j+d}) for every j∈[k]j\in[k] with j≥2j\ge2. Then Xj(s,t)=Xj+d(s′,t′)X_{j}(s,t)=X_{j+d}(s',t') for every j∈[k]j\in[k]. Indeed, let AA be the set of j∈Nj\in\mathbb{N} with j>kj>k or Xj(s,t)=Xj+d(s′,t′)X_{j}(s,t)=X_{j+d}(s',t'). Then 1∈A1\in A. If j∈Aj\in A and j+1≤kj+1\le k, then 2≤j+1+d≤k′2\le j+1+d\le k' and, by The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §nested,

Xj+1(s,t)=Eej+1(aj+1∗πej+1(Xj(s,t))bj+1)=Eej+1+d′(aj+1+d′∗πej+1+d′(Xj+d(s′,t′))bj+1+d′)=Xj+1+d(s′,t′);X_{j+1}(s,t)=E_{e_{j+1}}\bigl(a_{j+1}^{*}\pi_{e_{j+1}}(X_{j}(s,t))b_{j+1}\bigr)=E_{e'_{j+1+d}}\bigl(a'^{*}_{j+1+d}\pi_{e'_{j+1+d}}(X_{j+d}(s',t'))b'_{j+1+d}\bigr)=X_{j+1+d}(s',t');

if j+1>kj+1>k, then j+1∈Aj+1\in A trivially. So A=NA=\mathbb{N} by Principle of Induction for the Natural Numbers.

Claim 1 (vector space). By The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §space, sums and scalar multiples of elements of F\mathcal{F} lie in F\mathcal{F}, and the zero map lies in F\mathcal{F} (its support is empty). Two elements of F\mathcal{F} are equal when they agree at every label, and at a label ss each of conditions 1--8 of Vector Space over a Field reduces to the corresponding field identity in C\mathbb{C} (associativity and commutativity of addition, ξ(s)+0=ξ(s)\xi(s)+0=\xi(s), ξ(s)+(−1)ξ(s)=0\xi(s)+(-1)\xi(s)=0, λ(μξ(s))=(λμ)ξ(s)\lambda(\mu\xi(s))=(\lambda\mu)\xi(s), 1ξ(s)=ξ(s)1\xi(s)=\xi(s) and the two distributive laws), with the zero map as zero vector and (−1)ξ(-1)\xi as the vector ww of condition 4. So F\mathcal{F} is a complex vector space with zero vector the zero map.

(E) For every ξ∈F\xi\in\mathcal{F} and every nonempty finite F⊇supp⁡ξF\supseteq\operatorname{supp}\xi, ξ=∑s∈Fξ(s)δs\xi=\sum_{s\in F}\xi(s)\delta_{s}. At a label uu the right side takes the value ∑s∈Fξ(s)δs(u)\sum_{s\in F}\xi(s)\delta_{s}(u) (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §space). If u∈Fu\in F, the terms with s≠us\ne u vanish, so by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing and claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set the value is ξ(u)δu(u)=ξ(u)\xi(u)\delta_{u}(u)=\xi(u). If u∉Fu\notin F, all terms vanish, so the value is 00 (Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing), which is ξ(u)\xi(u) because u∉supp⁡ξu\notin\operatorname{supp}\xi. For ξ≠0\xi\ne0 the set supp⁡ξ\operatorname{supp}\xi is nonempty and finite, and (E) with F=supp⁡ξF=\operatorname{supp}\xi is the asserted expansion.

Claim 2 (symmetry of nested expectations). Let s=(a1,…,ak)s=(a_{1},\dots,a_{k}), t=(b1,…,bk)t=(b_{1},\dots,b_{k}) have type (e1,…,ek)(e_{1},\dots,e_{k}), and let AA be the set of j∈Nj\in\mathbb{N} with j>kj>k or Xj(t,s)=Xj(s,t)∗X_{j}(t,s)=X_{j}(s,t)^{*}. By The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §nested and the rules of the conventions,

X1(t,s)=Ee1(b1∗a1)=Ee1((a1∗b1)∗)=Ee1(a1∗b1)∗=X1(s,t)∗,X_{1}(t,s)=E_{e_{1}}(b_{1}^{*}a_{1})=E_{e_{1}}((a_{1}^{*}b_{1})^{*})=E_{e_{1}}(a_{1}^{*}b_{1})^{*}=X_{1}(s,t)^{*},

so 1∈A1\in A. Let j∈Aj\in A. If j+1>kj+1>k, then j+1∈Aj+1\in A. Otherwise Xj(t,s)=Xj(s,t)∗X_{j}(t,s)=X_{j}(s,t)^{*}, and with e=ej+1e=e_{j+1}

Xj+1(t,s)=Ee(bj+1∗πe(Xj(s,t)∗)aj+1)=Ee((aj+1∗πe(Xj(s,t))bj+1)∗)=Xj+1(s,t)∗.X_{j+1}(t,s)=E_{e}\bigl(b_{j+1}^{*}\pi_{e}(X_{j}(s,t)^{*})a_{j+1}\bigr)=E_{e}\bigl((a_{j+1}^{*}\pi_{e}(X_{j}(s,t))b_{j+1})^{*}\bigr)=X_{j+1}(s,t)^{*}.

So A=NA=\mathbb{N} by Principle of Induction for the Natural Numbers, which gives the claim for every j∈[k]j\in[k].

Claim 3 (positive Gram operators). HμM\mathcal{H}_{\mu}^{M} is a complex Hilbert space (Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §hilbert), so G∗∈L(HμM)G^{*}\in\mathcal{L}(\mathcal{H}_{\mu}^{M}) exists (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint), and by Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks and Claim 2 (with j=kj=k)

(G∗)rq=(Gqr)∗=Xk(tq,tr)∗=Xk(tr,tq)=Grq(r,q∈[M]).(G^{*})_{rq}=(G_{qr})^{*}=X_{k}(t^{q},t^{r})^{*}=X_{k}(t^{r},t^{q})=G_{rq}\qquad(r,q\in[M]).

By the uniqueness in Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks, G∗=GG^{*}=G; so GG is an adjoint of itself and hence self-adjoint (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). By Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation §maps it remains to show that GG is positive semi-definite (Positive Semi-Definite Operator). We use:

(G) Let e∈{1,2}e\in\{1,2\} and D∈L(HγeM)D\in\mathcal{L}(\mathcal{H}_{\gamma_{e}}^{M}) be such that, for all r,q∈[M]r,q\in[M], (D∗D)rq∈Ae(D^{*}D)_{rq}\in A_{e} and Grq=Ee((D∗D)rq)G_{rq}=E_{e}((D^{*}D)_{rq}). Then ⟨ζ,Gζ⟩\langle\zeta,G\zeta\rangle is a real number ≥0\ge0 for every ζ∈HμM\zeta\in\mathcal{H}_{\mu}^{M}. Here D∗D^{*} exists as above. Put η=(Veζ1,…,VeζM)∈HγeM\eta=(V_{e}\zeta_{1},\dots,V_{e}\zeta_{M})\in\mathcal{H}_{\gamma_{e}}^{M}. By Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks (twice), the identity for ⟨ζ,Ee(c)ζ′⟩\langle\zeta,E_{e}(c)\zeta'\rangle of the conventions, and 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,

⟨ζ,Gζ⟩=∑r=1M∑q=1M⟨ζr,Ee((D∗D)rq)ζq⟩=∑r=1M∑q=1M⟨Veζr,(D∗D)rqVeζq⟩=⟨η,D∗Dη⟩=∥Dη∥2≥0.\langle\zeta,G\zeta\rangle=\sum_{r=1}^{M}\sum_{q=1}^{M}\langle\zeta_{r},E_{e}((D^{*}D)_{rq})\zeta_{q}\rangle=\sum_{r=1}^{M}\sum_{q=1}^{M}\langle V_{e}\zeta_{r},(D^{*}D)_{rq}V_{e}\zeta_{q}\rangle=\langle\eta,D^{*}D\eta\rangle=\lVert D\eta\rVert^{2}\ge0.

Moreover, by Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks, (D∗D)rq=∑j=1M(Djr)∗Djq(D^{*}D)_{rq}=\sum_{j=1}^{M}(D_{jr})^{*}D_{jq} for every DD.

Let KK be the set of k∈Nk\in\mathbb{N} such that, for every M∈NM\in\mathbb{N} and all alternating tuples t1,…,tMt^{1},\dots,t^{M} of length kk and a common type, the operator GG of the claim is positive semi-definite.

1∈K1\in K. Let tr=((e,ar))t^{r}=((e,a^{r})) for r∈[M]r\in[M]. Let D∈L(HγeM)D\in\mathcal{L}(\mathcal{H}_{\gamma_{e}}^{M}) have blocks D1q=aqD_{1q}=a^{q} and Djq=0D_{jq}=0 for j≠1j\ne1 (Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks). The terms with j≠1j\ne1 of ∑j(Djr)∗Djq\sum_{j}(D_{jr})^{*}D_{jq} are 00, so by claim 7 of Properties of Finite Sums of Vectors, (D∗D)rq=(ar)∗aq∈Ae(D^{*}D)_{rq}=(a^{r})^{*}a^{q}\in A_{e}, and Grq=X1(tr,tq)=Ee((ar)∗aq)G_{rq}=X_{1}(t^{r},t^{q})=E_{e}((a^{r})^{*}a^{q}) (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §nested). By (G), GG is positive semi-definite.

k∈Kk\in K implies k+1∈Kk+1\in K. Let t1,…,tMt^{1},\dots,t^{M} have length k+1k+1 and common type (e1,…,ek+1)(e_{1},\dots,e_{k+1}); put e=ek+1e=e_{k+1}, let ara^{r} be the last entry of trt^{r}, and let srs^{r} be the alternating tuple of length kk and type (e1,…,ek)(e_{1},\dots,e_{k}) formed by the first kk entries of trt^{r}. By (X) with d=0d=0, Xk(sr,sq)=Xk(tr,tq)X_{k}(s^{r},s^{q})=X_{k}(t^{r},t^{q}). Let P∈L(HμM)P\in\mathcal{L}(\mathcal{H}_{\mu}^{M}) have blocks Prq=Xk(sr,sq)P_{rq}=X_{k}(s^{r},s^{q}); since k∈Kk\in K and PP is self-adjoint by the first paragraph, P≥0P\ge0. Each PrqP_{rq} lies in NN, so commutes with RpR_{p} for every p∈Pnp\in\mathcal{P}_{n} (The Tracial Algebra of a Noncommutative Law and Its Trace §algebra); by Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §diagonal, Rp(M)∈L(HμM)R_{p}^{(M)}\in\mathcal{L}(\mathcal{H}_{\mu}^{M}) commutes with PP. Let CC be given by Square Roots of Positive Bounded Operators on a Complex Hilbert Space, Commuting with Everything that Commutes with the Operator for PP: C≥0C\ge0, CC=PCC=P (Square Roots of Positive Bounded Operators on a Complex Hilbert Space, Commuting with Everything that Commutes with the Operator §square-root), and CC commutes with every Rp(M)R_{p}^{(M)} (Square Roots of Positive Bounded Operators on a Complex Hilbert Space, Commuting with Everything that Commutes with the Operator §commutation). By Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §diagonal, each block Crq∈L(Hμ)C_{rq}\in\mathcal{L}(\mathcal{H}_{\mu}) commutes with every RpR_{p}, i.e. Crq∈NC_{rq}\in N. As CC is self-adjoint, it is its own adjoint (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, 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), so Crq=(C∗)rq=(Cqr)∗C_{rq}=(C^{*})_{rq}=(C_{qr})^{*} and Prq=(CC)rq=∑j=1M(Cjr)∗CjqP_{rq}=(CC)_{rq}=\sum_{j=1}^{M}(C_{jr})^{*}C_{jq} (Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks). Let D∈L(HγeM)D\in\mathcal{L}(\mathcal{H}_{\gamma_{e}}^{M}) have blocks Djq=πe(Cjq)aq∈AeD_{jq}=\pi_{e}(C_{jq})a^{q}\in A_{e}. Then, using the properties of πe\pi_{e} and claim 4 of Properties of Finite Sums of Vectors for the linear map T↦(ar)∗πe(T)aqT\mapsto(a^{r})^{*}\pi_{e}(T)a^{q} on NN,

(D∗D)rq=∑j=1M(ar)∗πe(Cjr)∗πe(Cjq)aq=∑j=1M(ar)∗πe((Cjr)∗Cjq)aq=(ar)∗πe(Prq)aq∈Ae,(D^{*}D)_{rq}=\sum_{j=1}^{M}(a^{r})^{*}\pi_{e}(C_{jr})^{*}\pi_{e}(C_{jq})a^{q}=\sum_{j=1}^{M}(a^{r})^{*}\pi_{e}((C_{jr})^{*}C_{jq})a^{q}=(a^{r})^{*}\pi_{e}(P_{rq})a^{q}\in A_{e},

and Grq=Xk+1(tr,tq)=Ee((ar)∗πe(Xk(tr,tq))aq)=Ee((D∗D)rq)G_{rq}=X_{k+1}(t^{r},t^{q})=E_{e}\bigl((a^{r})^{*}\pi_{e}(X_{k}(t^{r},t^{q}))a^{q}\bigr)=E_{e}((D^{*}D)_{rq}). By (G), GG is positive semi-definite, so k+1∈Kk+1\in K.

By Principle of Induction for the Natural Numbers, K=NK=\mathbb{N}; with self-adjointness, G≥0G\ge0.

Claim 4 (the form). (H) For ξ,η∈F\xi,\eta\in\mathcal{F} and nonempty finite sets F⊇supp⁡ξF\supseteq\operatorname{supp}\xi, F′⊇supp⁡ηF'\supseteq\operatorname{supp}\eta,

h(ξ,η)=∑s∈F∑t∈F′ξ(s)‾ η(t) h0(s,t).h(\xi,\eta)=\sum_{s\in F}\sum_{t\in F'}\overline{\xi(s)}\,\eta(t)\,h_{0}(s,t).

If ξ=0\xi=0 or η=0\eta=0, every term vanishes and both sides are 00 (Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing, The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §form). Otherwise, for each ss the terms with t∉supp⁡ηt\notin\operatorname{supp}\eta vanish, and for s∉supp⁡ξs\notin\operatorname{supp}\xi the whole inner sum vanishes; two applications of Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing reduce the right side to the defining double sum over supp⁡ξ×supp⁡η\operatorname{supp}\xi\times\operatorname{supp}\eta.

Linearity in the second argument. With F=FξF=F_{\xi} and F′=Fη∪FζF'=F_{\eta}\cup F_{\zeta}, which contains supp⁡η\operatorname{supp}\eta, supp⁡ζ\operatorname{supp}\zeta and supp⁡(η+ζ)\operatorname{supp}(\eta+\zeta) (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §space) and is finite by claim 3 of Peeling an Element off a Finite Set, and Unions of Finite Sets, (H) and (S) give

h(ξ,η+ζ)=∑s∈F∑t∈F′ξ(s)‾ (η(t)+ζ(t)) h0(s,t)=h(ξ,η)+h(ξ,ζ).h(\xi,\eta+\zeta)=\sum_{s\in F}\sum_{t\in F'}\overline{\xi(s)}\,(\eta(t)+\zeta(t))\,h_{0}(s,t)=h(\xi,\eta)+h(\xi,\zeta).

Likewise, with F′=Fη⊇supp⁡(cη)F'=F_{\eta}\supseteq\operatorname{supp}(c\eta), (H) and (S) give h(ξ,cη)=c h(ξ,η)h(\xi,c\eta)=c\,h(\xi,\eta).

Hermitian symmetry. First, h0(t,s)=h0(s,t)‾h_{0}(t,s)=\overline{h_{0}(s,t)} for all labels s,ts,t. For NN-labels s=(0,x)s=(0,x), t=(0,y)t=(0,y), 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, h0(t,s)=τμ(y∗x)=τμ((x∗y)∗)=τμ(x∗y)‾h_{0}(t,s)=\tau_{\mu}(y^{*}x)=\tau_{\mu}((x^{*}y)^{*})=\overline{\tau_{\mu}(x^{*}y)}. For tuples of the same length kk and type, by Claim 2 and 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, h0(t,s)=τμ(Xk(s,t)∗)=τμ(Xk(s,t))‾h_{0}(t,s)=\tau_{\mu}(X_{k}(s,t)^{*})=\overline{\tau_{\mu}(X_{k}(s,t))}. For all other pairs both values are 00, as the condition in (Z) is symmetric. Now take F=FξF=F_{\xi}, F′=FηF'=F_{\eta}. By (H), claim 5 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set (interchange), and Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §conjugate with the rules for conjugates of products,

h(η,ξ)=∑s∈F∑t∈F′η(t)‾ ξ(s) h0(s,t)‾=∑s∈F∑t∈F′ξ(s)‾ η(t) h0(s,t)‾=h(ξ,η)‾.h(\eta,\xi)=\sum_{s\in F}\sum_{t\in F'}\overline{\eta(t)}\,\xi(s)\,\overline{h_{0}(s,t)}=\overline{\sum_{s\in F}\sum_{t\in F'}\overline{\xi(s)}\,\eta(t)\,h_{0}(s,t)}=\overline{h(\xi,\eta)}.

Basis values. δs,δt≠0\delta_{s},\delta_{t}\ne0 with supports {s}\{s\}, {t}\{t\}, so by The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §form and claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, h(δs,δt)=1‾⋅1⋅h0(s,t)=h0(s,t)h(\delta_{s},\delta_{t})=\overline{1}\cdot1\cdot h_{0}(s,t)=h_{0}(s,t).

Positivity. If ξ=0\xi=0, then h(ξ,ξ)=0h(\xi,\xi)=0. Let ξ≠0\xi\ne0, F=supp⁡ξF=\operatorname{supp}\xi, and f(s,t)=ξ(s)‾ ξ(t) h0(s,t)f(s,t)=\overline{\xi(s)}\,\xi(t)\,h_{0}(s,t). Let κ((0,x))=0\kappa((0,x))=0 and κ(t)=(k,type of t)\kappa(t)=(k,\text{type of }t) for a tuple tt of length kk; by (Z), h0(s,t)=0h_{0}(s,t)=0 if κ(s)≠κ(t)\kappa(s)\ne\kappa(t). The set Γ={κ(s):s∈F}\Gamma=\{\kappa(s):s\in F\} is nonempty and finite (claim 4 of Basic Properties of Finite Sets), and each Fγ={s∈F:κ(s)=γ}F_{\gamma}=\{s\in F:\kappa(s)=\gamma\}, γ∈Γ\gamma\in\Gamma, is nonempty and finite. For s∈Fγs\in F_{\gamma}, ∑t∈Ff(s,t)=∑t∈Fγf(s,t)\sum_{t\in F}f(s,t)=\sum_{t\in F_{\gamma}}f(s,t) by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing. The map (γ,s)↦s(\gamma,s)\mapsto s is a bijection from the set of pairs (γ,s)(\gamma,s) with γ∈Γ\gamma\in\Gamma, s∈Fγs\in F_{\gamma} onto FF (inverse s↦(κ(s),s)s\mapsto(\kappa(s),s)), so by Sum over a Finite Index Set (composing bijections) and Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §pairs,

h(ξ,ξ)=∑γ∈ΓQγ,Qγ=∑s∈Fγ∑t∈Fγf(s,t).h(\xi,\xi)=\sum_{\gamma\in\Gamma}Q_{\gamma},\qquad Q_{\gamma}=\sum_{s\in F_{\gamma}}\sum_{t\in F_{\gamma}}f(s,t).

Each QγQ_{\gamma} is a real number ≥0\ge0. Enumerate FγF_{\gamma} by a bijection from [M][M] and compute the sums along it (Sum over a Finite Index Set). If γ=0\gamma=0, write F0={(0,x1),…,(0,xM)}F_{0}=\{(0,x_{1}),\dots,(0,x_{M})\} and cr=ξ((0,xr))c_{r}=\xi((0,x_{r})); by The Tracial Algebra of a Noncommutative Law and Its Trace §trace, the defining property of the adjoint, and claim 2 of Elementary Properties of a Complex Inner Product, cr‾cqτμ(xr∗xq)=cr‾cq⟨xrΩμ,xqΩμ⟩=⟨yr,yq⟩\overline{c_{r}}c_{q}\tau_{\mu}(x_{r}^{*}x_{q})=\overline{c_{r}}c_{q}\langle x_{r}\Omega_{\mu},x_{q}\Omega_{\mu}\rangle=\langle y_{r},y_{q}\rangle with yr=crxrΩμy_{r}=c_{r}x_{r}\Omega_{\mu}, so by claim 5 of Properties of Finite Sums of Vectors (twice) Q0=⟨y,y⟩=∥y∥2≥0Q_{0}=\langle y,y\rangle=\lVert y\rVert^{2}\ge0 with y=∑r=1Myry=\sum_{r=1}^{M}y_{r}. If γ=(k,e)\gamma=(k,e), write Fγ={t1,…,tM}F_{\gamma}=\{t^{1},\dots,t^{M}\}, tuples of length kk and common type ee, and cr=ξ(tr)c_{r}=\xi(t^{r}); with GG as in Claim 3 and ζ=(c1Ωμ,…,cMΩμ)∈HμM\zeta=(c_{1}\Omega_{\mu},\dots,c_{M}\Omega_{\mu})\in\mathcal{H}_{\mu}^{M}, The Tracial Algebra of a Noncommutative Law and Its Trace §trace, claim 2 of Elementary Properties of a Complex Inner Product and Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators §blocks give

Qγ=∑r=1M∑q=1Mcr‾cq τμ(Xk(tr,tq))=∑r=1M∑q=1M⟨crΩμ,Grq(cqΩμ)⟩=⟨ζ,Gζ⟩,Q_{\gamma}=\sum_{r=1}^{M}\sum_{q=1}^{M}\overline{c_{r}}c_{q}\,\tau_{\mu}(X_{k}(t^{r},t^{q}))=\sum_{r=1}^{M}\sum_{q=1}^{M}\langle c_{r}\Omega_{\mu},G_{rq}(c_{q}\Omega_{\mu})\rangle=\langle\zeta,G\zeta\rangle,

a real number ≥0\ge0 by Claim 3 and Positive Semi-Definite Operator. Hence h(ξ,ξ)h(\xi,\xi) is a sum of nonnegative real numbers, a real number ≥0\ge0 by Nonnegativity and Monotonicity of a Sum over a Finite Index Set §nonnegative.

Claim 5 (formal actions). Write ρb=ρε,b\rho_{b}=\rho_{\varepsilon,b}, ℓ(b)=ℓε(b)\ell(b)=\ell_{\varepsilon}(b), π=πε\pi=\pi_{\varepsilon}, E=EεE=E_{\varepsilon}. (L) For ξ∈F\xi\in\mathcal{F} and nonempty finite F⊇supp⁡ξF\supseteq\operatorname{supp}\xi, ℓ(b)ξ=∑u∈Fξ(u)ρb(u)\ell(b)\xi=\sum_{u\in F}\xi(u)\rho_{b}(u): at each label the terms with u∉supp⁡ξu\notin\operatorname{supp}\xi vanish, so by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §vanishing the value agrees with The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §actions (both are 00 if ξ=0\xi=0). With F=Fξ∪FηF=F_{\xi}\cup F_{\eta}, (L) and (S) evaluated at each label give ℓ(b)(ξ+η)=ℓ(b)ξ+ℓ(b)η\ell(b)(\xi+\eta)=\ell(b)\xi+\ell(b)\eta; with F=FξF=F_{\xi} they give ℓ(b)(cξ)=c ℓ(b)ξ\ell(b)(c\xi)=c\,\ell(b)\xi. So ℓ(b)\ell(b) is linear (Linear Map, Claim 1). By (L) with F={u}F=\{u\} and claim 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, ℓ(b)δu=ρb(u)\ell(b)\delta_{u}=\rho_{b}(u).

(B) Let U,WU,W be nonempty finite sets, c:U→Cc:U\to\mathbb{C}, d:W→Cd:W\to\mathbb{C}, φ:U→F\varphi:U\to\mathcal{F}, ψ:W→F\psi:W\to\mathcal{F}. Then

h(∑u∈Uc(u)φ(u),∑w∈Wd(w)ψ(w))=∑u∈U∑w∈Wc(u)‾ d(w) h(φ(u),ψ(w)).h\Bigl(\sum_{u\in U}c(u)\varphi(u),\sum_{w\in W}d(w)\psi(w)\Bigr)=\sum_{u\in U}\sum_{w\in W}\overline{c(u)}\,d(w)\,h(\varphi(u),\psi(w)).

Let SS be the union of {o}\{o\}, of the sets supp⁡φ(u)\operatorname{supp}\varphi(u) and of the sets supp⁡ψ(w)\operatorname{supp}\psi(w); it is finite by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §finite-union and claims 1 and 3 of Peeling an Element off a Finite Set, and Unions of Finite Sets, and it contains the supports of both combinations (The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §space). Apply (H) with F=F′=SF=F'=S to the left side; expand the conjugate of the first combination at ss by Sums over Finite Index Sets: Finite Unions, Disjoint Unions, Vanishing Terms, Dependent Pairs, Conjugation and the Modulus §conjugate, multiply out by (S), interchange the sums over SS with those over UU and WW (claim 5 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set), and pull out c(u)‾d(w)\overline{c(u)}d(w) by (S); the remaining double sum over S×SS\times S is h(φ(u),ψ(w))h(\varphi(u),\psi(w)) by (H).

(D2) For labels u1,u2,vu_{1},u_{2},v: h(δu1+δu2,δv)=h0(u1,v)+h0(u2,v)h(\delta_{u_{1}}+\delta_{u_{2}},\delta_{v})=h_{0}(u_{1},v)+h_{0}(u_{2},v) and h(δv,δu1+δu2)=h0(v,u1)+h0(v,u2)h(\delta_{v},\delta_{u_{1}}+\delta_{u_{2}})=h_{0}(v,u_{1})+h_{0}(v,u_{2}). The second is additivity and the basis values of Claim 4; the first follows from it by Hermitian symmetry and h0(u,v)=h0(v,u)‾h_{0}(u,v)=\overline{h_{0}(v,u)} (Claim 4).

Reduction. Let ξ,η∈F\xi,\eta\in\mathcal{F}. By (E), (L), (B) (with U=FξU=F_{\xi}, W=FηW=F_{\eta}) and b∗∈Aεb^{*}\in A_{\varepsilon},

h(ℓ(b)ξ,η)=∑u∈Fξ∑v∈Fηξ(u)‾ η(v) h(ρb(u),δv),h(ξ,ℓ(b∗)η)=∑u∈Fξ∑v∈Fηξ(u)‾ η(v) h(δu,ρb∗(v)),h(\ell(b)\xi,\eta)=\sum_{u\in F_{\xi}}\sum_{v\in F_{\eta}}\overline{\xi(u)}\,\eta(v)\,h(\rho_{b}(u),\delta_{v}),\qquad h(\xi,\ell(b^{*})\eta)=\sum_{u\in F_{\xi}}\sum_{v\in F_{\eta}}\overline{\xi(u)}\,\eta(v)\,h(\delta_{u},\rho_{b^{*}}(v)),

so it suffices to prove, for all labels u,vu,v, the statement (⋆)(u,v)(\star)(u,v): h(ρb(u),δv)=h(δu,ρb∗(v))h(\rho_{b}(u),\delta_{v})=h(\delta_{u},\rho_{b^{*}}(v)) for every b∈Aεb\in A_{\varepsilon}. If (⋆)(u,v)(\star)(u,v) holds, so does (⋆)(v,u)(\star)(v,u): for b∈Aεb\in A_{\varepsilon}, (⋆)(u,v)(\star)(u,v) for b∗b^{*} gives h(ρb∗(u),δv)=h(δu,ρb(v))h(\rho_{b^{*}}(u),\delta_{v})=h(\delta_{u},\rho_{b}(v)) (as b∗∗=bb^{**}=b), and conjugating with Hermitian symmetry gives h(δv,ρb∗(u))=h(ρb(v),δu)h(\delta_{v},\rho_{b^{*}}(u))=h(\rho_{b}(v),\delta_{u}). Every label is an NN-label, a tuple whose type starts with ε\varepsilon, or one whose type starts with εˉ\bar{\varepsilon}; so it suffices to treat the six cases below. Each side is evaluated by The Formal Amalgamated Free Product over a Common Marginal: Alternating Tuples, the Free Vector Space, the Nested-Expectation Form and the Formal Actions §actions and (D2), and terms are discarded by (Z).

Case u=(0,x)u=(0,x), v=(0,y)v=(0,y). Left side: h0((0,E(bπ(x))),(0,y))=τμ(E(bπ(x))∗y)=τμ(x∗E(b∗)y)h_{0}((0,E(b\pi(x))),(0,y))=\tau_{\mu}(E(b\pi(x))^{*}y)=\tau_{\mu}(x^{*}E(b^{*})y), since E(bπ(x))∗=E(π(x∗)b∗)=x∗E(b∗)E(b\pi(x))^{*}=E(\pi(x^{*})b^{*})=x^{*}E(b^{*}). Right side: h0((0,x),(0,E(b∗π(y))))=τμ(x∗E(b∗)y)h_{0}((0,x),(0,E(b^{*}\pi(y))))=\tau_{\mu}(x^{*}E(b^{*})y). The pairings involving the 11-tuples vanish.

Case u=(0,x)u=(0,x), v=t=(a1,…,ak)v=t=(a_{1},\dots,a_{k}), type starting with ε\varepsilon. If k≥2k\ge2, both sides vanish: ρb(u)\rho_{b}(u) consists of a 11-tuple and an NN-label, and ρb∗(t)\rho_{b^{*}}(t) of two tuples. If k=1k=1, by (C) (as a1∈Aε∘a_{1}\in A_{\varepsilon}^{\circ}) the left side is

h0(((ε,(bπ(x))∘)),t)=τμ(E(((bπ(x))∘)∗a1))=τμ(E(π(x∗)b∗a1))=τμ(x∗E(b∗a1)),h_{0}\bigl(((\varepsilon,(b\pi(x))^{\circ})),t\bigr)=\tau_{\mu}\bigl(E(((b\pi(x))^{\circ})^{*}a_{1})\bigr)=\tau_{\mu}\bigl(E(\pi(x^{*})b^{*}a_{1})\bigr)=\tau_{\mu}(x^{*}E(b^{*}a_{1})),

and the right side is h0((0,x),(0,E(b∗a1)))=τμ(x∗E(b∗a1))h_{0}((0,x),(0,E(b^{*}a_{1})))=\tau_{\mu}(x^{*}E(b^{*}a_{1})).

Case u=(0,x)u=(0,x), v=tv=t with type starting with εˉ\bar{\varepsilon}. The 11-tuple in ρb(u)\rho_{b}(u) has type (ε)(\varepsilon), and ρb∗(t)\rho_{b^{*}}(t) consists of two tuples; both sides are 00.

Case u=s=((e1,a1),…,(ek,ak))u=s=((e_{1},a_{1}),\dots,(e_{k},a_{k})), v=t=((e1′,a1′),…,(el′,al′))v=t=((e'_{1},a'_{1}),\dots,(e'_{l},a'_{l})), e1=e1′=εe_{1}=e'_{1}=\varepsilon. By clause (c), ρb(s)=δs′+δw\rho_{b}(s)=\delta_{s'}+\delta_{w} with s′=((ε,(ba1)∘),(e2,a2),…,(ek,ak))s'=((\varepsilon,(ba_{1})^{\circ}),(e_{2},a_{2}),\dots,(e_{k},a_{k})) of the type of ss, and ww an NN-label (k=1k=1) or a tuple of type starting with e2=εˉe_{2}=\bar{\varepsilon}; likewise ρb∗(t)=δt′+δw′\rho_{b^{*}}(t)=\delta_{t'}+\delta_{w'} with t′=((ε,(b∗a1′)∘),(e2′,a2′),… )t'=((\varepsilon,(b^{*}a'_{1})^{\circ}),(e'_{2},a'_{2}),\dots) of the type of tt. So the left side is h0(s′,t)h_{0}(s',t) and the right side h0(s,t′)h_{0}(s,t'), both 00 unless l=kl=k and s,ts,t have the same type. In that case, by (C) (as a1,a1′∈Aε∘a_{1},a'_{1}\in A_{\varepsilon}^{\circ}), X1(s′,t)=E(a1∗b∗a1′)=X1(s,t′)X_{1}(s',t)=E(a_{1}^{*}b^{*}a'_{1})=X_{1}(s,t'), and the pairs (s′,t)(s',t), (s,t′)(s,t') have the same entries in positions j≥2j\ge2; so Xk(s′,t)=Xk(s,t′)X_{k}(s',t)=X_{k}(s,t') by (X) with d=0d=0, and the sides agree.

Case u=su=s as before (e1=εe_{1}=\varepsilon), v=t=((e1′,a1′),…,(el′,al′))v=t=((e'_{1},a'_{1}),\dots,(e'_{l},a'_{l})), e1′=εˉe'_{1}=\bar{\varepsilon}. With ρb(s)=δs′+δw\rho_{b}(s)=\delta_{s'}+\delta_{w} as before, h0(s′,t)=0h_{0}(s',t)=0. By clause (b), ρb∗(t)=δt++δt−\rho_{b^{*}}(t)=\delta_{t^{+}}+\delta_{t^{-}} with t+=((ε,(b∗)∘),(e1′,a1′),…,(el′,al′))t^{+}=((\varepsilon,(b^{*})^{\circ}),(e'_{1},a'_{1}),\dots,(e'_{l},a'_{l})) and t−t^{-} of the type of tt, so h0(s,t−)=0h_{0}(s,t^{-})=0. The left side is h0(w,t)h_{0}(w,t), the right side h0(s,t+)h_{0}(s,t^{+}). If k≥2k\ge2, w=((e2,πe2(E(ba1))a2),(e3,a3),…,(ek,ak))w=((e_{2},\pi_{e_{2}}(E(ba_{1}))a_{2}),(e_{3},a_{3}),\dots,(e_{k},a_{k})) has length k−1k-1 and type (e2,…,ek)(e_{2},\dots,e_{k}); so both sides vanish unless (†\dagger) k=l+1k=l+1 and (e2,…,ek)=(e1′,…,el′)(e_{2},\dots,e_{k})=(e'_{1},\dots,e'_{l}) (if k=1k=1, ww is an NN-label and (†\dagger) fails as l≥1l\ge1). Under (†\dagger), by (C) (as a1∈Aε∘a_{1}\in A_{\varepsilon}^{\circ}) X1(s,t+)=E(a1∗b∗)X_{1}(s,t^{+})=E(a_{1}^{*}b^{*}), so, as E(ba1)∗=E(a1∗b∗)E(ba_{1})^{*}=E(a_{1}^{*}b^{*}),

X2(s,t+)=Ee2(a2∗πe2(E(a1∗b∗))a1′)=Ee2((πe2(E(ba1))a2)∗a1′)=X1(w,t),X_{2}(s,t^{+})=E_{e_{2}}\bigl(a_{2}^{*}\pi_{e_{2}}(E(a_{1}^{*}b^{*}))a'_{1}\bigr)=E_{e_{2}}\bigl((\pi_{e_{2}}(E(ba_{1}))a_{2})^{*}a'_{1}\bigr)=X_{1}(w,t),

and for 2≤j≤k−12\le j\le k-1 the jj-th entries of w,tw,t are (ej+1,aj+1)(e_{j+1},a_{j+1}), (ej+1,aj′)(e_{j+1},a'_{j}), the (j+1)(j+1)-th entries of s,t+s,t^{+}. By (X) with d=1d=1, Xk−1(w,t)=Xk(s,t+)X_{k-1}(w,t)=X_{k}(s,t^{+}), and the sides agree.

Case u=s=((e1,a1),… )u=s=((e_{1},a_{1}),\dots), v=t=((e1′,a1′),… )v=t=((e'_{1},a'_{1}),\dots), e1=e1′=εˉe_{1}=e'_{1}=\bar{\varepsilon}. By clause (b), ρb(s)=δs++δs−\rho_{b}(s)=\delta_{s^{+}}+\delta_{s^{-}} and ρb∗(t)=δt++δt−\rho_{b^{*}}(t)=\delta_{t^{+}}+\delta_{t^{-}}, where s+,t+s^{+},t^{+} have types starting with ε\varepsilon and s−=((e1,πe1(E(b))a1),(e2,a2),… )s^{-}=((e_{1},\pi_{e_{1}}(E(b))a_{1}),(e_{2},a_{2}),\dots), t−=((e1′,πe1(E(b∗))a1′),(e2′,a2′),… )t^{-}=((e'_{1},\pi_{e_{1}}(E(b^{*}))a'_{1}),(e'_{2},a'_{2}),\dots) have the types of ss, tt. So the left side is h0(s−,t)h_{0}(s^{-},t) and the right side h0(s,t−)h_{0}(s,t^{-}), both 00 unless s,ts,t have the same length kk and type. In that case, as E(b)∗=E(b∗)E(b)^{*}=E(b^{*}),

X1(s−,t)=Ee1(a1∗πe1(E(b))∗a1′)=Ee1(a1∗πe1(E(b∗))a1′)=X1(s,t−),X_{1}(s^{-},t)=E_{e_{1}}\bigl(a_{1}^{*}\pi_{e_{1}}(E(b))^{*}a'_{1}\bigr)=E_{e_{1}}\bigl(a_{1}^{*}\pi_{e_{1}}(E(b^{*}))a'_{1}\bigr)=X_{1}(s,t^{-}),

the later entries coincide, and (X) with d=0d=0 gives Xk(s−,t)=Xk(s,t−)X_{k}(s^{-},t)=X_{k}(s,t^{-}).

In all cases (⋆)(\star) holds, which proves h(ℓε(b)ξ,η)=h(ξ,ℓε(b∗)η)h(\ell_{\varepsilon}(b)\xi,\eta)=h(\xi,\ell_{\varepsilon}(b^{*})\eta).

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