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

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Affine tuples are self-adjoint because their coefficients are real, so affine substitutions are unital *-homomorphisms that pull tracial states and laws back; composition and the moment and coordinate formulas follow by expanding finite sums, comparing coefficients and using traciality.

Proof

Each result cited below is universally quantified over the data in its own statement. For k∈Nk\in\mathbb{N} the space Pk\mathcal{P}_{k} is a complex vector space by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §vector-space, and finite sums in it are those of Finite Sum Notation in a Vector Space. We use the rules of Properties of Finite Sums of Vectors for such sums (claim 1: recursion; claim 2: additivity; claim 3: homogeneity; claim 4: a linear map commutes with a finite sum; claim 7: a single possibly nonzero summand) and the same rules for finite sums of numbers, claims 1, 2, 3 and 7 of Properties of Finite Sums. For p∈Pkp\in\mathcal{P}_{k} the maps q↦pqq\mapsto pq and q↦qpq\mapsto qp of Pk\mathcal{P}_{k} into itself are linear by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra; composing with a linear map λ:Pk→C\lambda:\mathcal{P}_{k}\to\mathbb{C}, so are q↦λ(pq)q\mapsto\lambda(pq) and q↦λ(qp)q\mapsto\lambda(qp). We call this fact (L). For an affine datum UU with tuple aUa^{U}, the map σU=σaU\sigma_{U}=\sigma_{a^{U}} is linear by Substitution of Noncommutative Polynomials into the Variables §substitution, and by Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §values and Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §homomorphism (for the tuple aUa^{U}) it satisfies σU(1)=1\sigma_{U}(1)=1, σU(xj)=ajU\sigma_{U}(x_{j})=a^{U}_{j} and σU(pq)=σU(p)σU(q)\sigma_{U}(pq)=\sigma_{U}(p)\sigma_{U}(q). We call these facts (H).

Proof of clause 1 (Self-adjointness). Let i∈[n]i\in[n]. By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §self-adjoint, Pm,sa\mathcal{P}_{m,\mathrm{sa}} contains 11 and x1,…,xmx_{1},\dots,x_{m} and is closed under sums and under multiplication by real numbers. Since cic_{i} and the AijA_{ij} are real, ci1c_{i}1 and each AijxjA_{ij}x_{j} are self-adjoint; by induction on k∈[m]k\in[m] along the recursion of claim 1 of Properties of Finite Sums of Vectors, each partial sum ∑j=1kAijxj\sum_{j=1}^{k}A_{ij}x_{j} is self-adjoint, and hence so is aiTa^{T}_{i}. Thus aTa^{T} is an nn-tuple in Pm,sa\mathcal{P}_{m,\mathrm{sa}}.

Let λ\lambda be a tracial state on Pm\mathcal{P}_{m} and put λT=λ∘σT\lambda_{T}=\lambda\circ\sigma_{T}, a linear map Pn→C\mathcal{P}_{n}\to\mathbb{C} as a composite of linear maps. Since aTa^{T} is self-adjoint, Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §adjoint gives σT(p∗)=σT(p)∗\sigma_{T}(p^{*})=\sigma_{T}(p)^{*} for p∈Pnp\in\mathcal{P}_{n}. Let p,q∈Pnp,q\in\mathcal{P}_{n}. By (H) and the three conditions of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state for λ\lambda: λT(1)=λ(1)=1\lambda_{T}(1)=\lambda(1)=1; λT(p∗p)=λ(σT(p)∗σT(p))\lambda_{T}(p^{*}p)=\lambda\bigl(\sigma_{T}(p)^{*}\sigma_{T}(p)\bigr) is real and nonnegative; and λT(pq)=λ(σT(p)σT(q))=λ(σT(q)σT(p))=λT(qp)\lambda_{T}(pq)=\lambda\bigl(\sigma_{T}(p)\sigma_{T}(q)\bigr)=\lambda\bigl(\sigma_{T}(q)\sigma_{T}(p)\bigr)=\lambda_{T}(qp). Hence λT\lambda_{T} is a tracial state on Pn\mathcal{P}_{n} by Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state.

Now let λ∈Σm\lambda\in\Sigma_{m}; by Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §law there is a real R>0R>0 with λ∈Σm,R\lambda\in\Sigma_{m,R}. For i∈[n]i\in[n] put si=∣ci∣+R∑j=1m∣Aij∣s_{i}=|c_{i}|+R\sum_{j=1}^{m}|A_{ij}|. Each ∣Aij∣|A_{ij}| and ∣ci∣|c_{i}| is nonnegative by claim 1 of Properties of the Absolute Value in an Ordered Field, so ∑j∣Aij∣≥0\sum_{j}|A_{ij}|\ge0 by claim 5 of Properties of Finite Sums, and si≥0s_{i}\ge0 by claims 5 and 2 of Elementary Arithmetic in an Ordered Field. Put S=1+∑i=1nsiS=1+\sum_{i=1}^{n}s_{i}. By claims 5 and 6 of Properties of Finite Sums, 0≤si≤∑k=1nsk0\le s_{i}\le\sum_{k=1}^{n}s_{k}, so by claims 1, 2 and 3 of Elementary Arithmetic in an Ordered Field we get si≤Ss_{i}\le S for every i∈[n]i\in[n] and 1≤S1\le S; hence S>0S>0 by claims 6 and 2 of Elementary Order Arithmetic in an Ordered Field. The tuple aTa^{T} has the form required in The Norm Bound of a Noncommutative Law: Multiplication by a Variable is Bounded, the Bound is Detected by Even Moments, and Laws Pull Back under Self-Adjoint Substitutions §affine (for the law λ∈Σm,R\lambda\in\Sigma_{m,R}, with d=md=m, coefficients ci0=cic_{i0}=c_{i} and cik=Aikc_{ik}=A_{ik}, and the bound SS), so that clause gives λ∘σT∈Σn,S⊆Σn\lambda\circ\sigma_{T}\in\Sigma_{n,S}\subseteq\Sigma_{n}.

Proof of clause 2 (Composition). Write S=(B,b)S=(B,b), so that aiS=bi1+∑j=1nBijxj∈Pna^{S}_{i}=b_{i}1+\sum_{j=1}^{n}B_{ij}x_{j}\in\mathcal{P}_{n} for i∈[r]i\in[r]. Let ee be the rr-tuple in Pm\mathcal{P}_{m} with ei=σT(aiS)e_{i}=\sigma_{T}(a^{S}_{i}). By Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §composition, applied to the rr-tuple aSa^{S} in Pn\mathcal{P}_{n} and the nn-tuple aTa^{T} in Pm\mathcal{P}_{m}, we have σT(σS(p))=σe(p)\sigma_{T}(\sigma_{S}(p))=\sigma_{e}(p) for every p∈Prp\in\mathcal{P}_{r}. By linearity of σT\sigma_{T}, claim 4 of Properties of Finite Sums of Vectors and (H),

ei=bi1+∑j=1nBij(cj1+∑l=1mAjlxl),e_{i}=b_{i}1+\sum_{j=1}^{n}B_{ij}\Bigl(c_{j}1+\sum_{l=1}^{m}A_{jl}x_{l}\Bigr),

while by Affine Data and Affine Substitutions of Noncommutative Polynomials §composite and Affine Data and Affine Substitutions of Noncommutative Polynomials §tuple

aiS∘T=(bi+∑j=1nBijcj)1+∑l=1m(∑j=1nBijAjl)xl.a^{S\circ T}_{i}=\Bigl(b_{i}+\sum_{j=1}^{n}B_{ij}c_{j}\Bigr)1+\sum_{l=1}^{m}\Bigl(\sum_{j=1}^{n}B_{ij}A_{jl}\Bigr)x_{l}.

Fix a word v∈Wmv\in W_{m}. The map p↦p(v)p\mapsto p(v) from Pm\mathcal{P}_{m} to C\mathbb{C} is linear, because the linear operations of The Algebra of Noncommutative Polynomials in Finitely Many Self-Adjoint Variables §linear act coefficientwise. Applying it, with claim 4 of Properties of Finite Sums of Vectors and claims 2 and 3 of Properties of Finite Sums, and writing ϵ=1(v)\epsilon=1(v) and ϵl=xl(v)\epsilon_{l}=x_{l}(v), we get

ei(v)=biϵ+(∑j=1nBijcj)ϵ+∑j=1n∑l=1mBijAjlϵl,aiS∘T(v)=biϵ+(∑j=1nBijcj)ϵ+∑l=1m∑j=1nBijAjlϵl.e_{i}(v)=b_{i}\epsilon+\Bigl(\sum_{j=1}^{n}B_{ij}c_{j}\Bigr)\epsilon+\sum_{j=1}^{n}\sum_{l=1}^{m}B_{ij}A_{jl}\epsilon_{l},\qquad a^{S\circ T}_{i}(v)=b_{i}\epsilon+\Bigl(\sum_{j=1}^{n}B_{ij}c_{j}\Bigr)\epsilon+\sum_{l=1}^{m}\sum_{j=1}^{n}B_{ij}A_{jl}\epsilon_{l}.

These agree by Interchange of a Finite Double Sum, applied in C\mathbb{C} to the nn-tuple of mm-tuples with components BijAjlϵlB_{ij}A_{jl}\epsilon_{l}. Polynomials are maps Wm→CW_{m}\to\mathbb{C} by The Algebra of Noncommutative Polynomials in Finitely Many Self-Adjoint Variables §polynomials, so ei=aiS∘Te_{i}=a^{S\circ T}_{i} for every i∈[r]i\in[r]. Hence σT∘σS=σe=σaS∘T=σS∘T\sigma_{T}\circ\sigma_{S}=\sigma_{e}=\sigma_{a^{S\circ T}}=\sigma_{S\circ T}.

For the identity datum, aiidm=0⋅1+∑j=1mEijxja^{\mathrm{id}_{m}}_{i}=0\cdot1+\sum_{j=1}^{m}E_{ij}x_{j}. The summands with j≠ij\neq i are 0xj=00x_{j}=0 and the summand with j=ij=i is xix_{i}, so claim 7 of Properties of Finite Sums of Vectors gives aiidm=xia^{\mathrm{id}_{m}}_{i}=x_{i}. Thus aidma^{\mathrm{id}_{m}} is the tuple x=(x1,…,xm)x=(x_{1},\dots,x_{m}) of variables, and σidm=σx\sigma_{\mathrm{id}_{m}}=\sigma_{x} is the identity map of Pm\mathcal{P}_{m} by Substitution is the Unique Unital Homomorphism with Prescribed Values on the Variables: Monomials, Products, Adjoints and Composition §identity. Finally, for a tracial state λ\lambda on Pm\mathcal{P}_{m}, associativity of composition of maps gives (λ∘σT)∘σS=λ∘(σT∘σS)=λ∘σS∘T(\lambda\circ\sigma_{T})\circ\sigma_{S}=\lambda\circ(\sigma_{T}\circ\sigma_{S})=\lambda\circ\sigma_{S\circ T} and λ∘σidm=λ\lambda\circ\sigma_{\mathrm{id}_{m}}=\lambda.

Proof of clause 3 (Moments). Let i,j∈[m]i,j\in[m]. The variables 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. Hence mi(λ)\mathrm{m}_{i}(\lambda) is real by Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §adjoint, and mij(λ)\mathrm{m}_{ij}(\lambda) is real by Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §pairing (both for the tracial state λ\lambda). Condition (c) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state gives mij(λ)=mji(λ)\mathrm{m}_{ij}(\lambda)=\mathrm{m}_{ji}(\lambda). By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §adjoint and Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §monomials, 1∗=11^{*}=1, xi∗=xix_{i}^{*}=x_{i}, 1xi=xi1x_{i}=x_{i} and 1∗1=11^{*}1=1. So Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §cauchy-schwarz with p=xip=x_{i} and q=1q=1 gives ∣λ(xi)∣2≤λ(xixi)λ(1)=mii(λ)|\lambda(x_{i})|^{2}\le\lambda(x_{i}x_{i})\lambda(1)=\mathrm{m}_{ii}(\lambda). Since mi(λ)\mathrm{m}_{i}(\lambda) is real, its modulus is its absolute value by claim 8 of Properties of the Absolute Value in an Ordered Field. That absolute value equals mi(λ)\mathrm{m}_{i}(\lambda) or −mi(λ)-\mathrm{m}_{i}(\lambda) by claim 1 of the same lemma, so its square is mi(λ)2\mathrm{m}_{i}(\lambda)^{2}, and mi(λ)2≤mii(λ)\mathrm{m}_{i}(\lambda)^{2}\le\mathrm{m}_{ii}(\lambda).

For real ξ1,…,ξm\xi_{1},\dots,\xi_{m} put a=∑i=1mξixia=\sum_{i=1}^{m}\xi_{i}x_{i}, which is self-adjoint by the argument of clause 1. By Basic Properties of Noncommutative Laws: Adjoints, the Self-Adjoint Pairing, Cauchy-Schwarz, Monotonicity in the Bound, and Laws of Constant Tuples §pairing, βλ(u,v)=λ(uv)\beta_{\lambda}(u,v)=\lambda(uv) is symmetric and bilinear over R\mathbb{R} on Pm,sa\mathcal{P}_{m,\mathrm{sa}}. Applying claim 4 of Properties of Finite Sums of Vectors to the linear maps u↦βλ(u,a)u\mapsto\beta_{\lambda}(u,a) and v↦βλ(xi,v)v\mapsto\beta_{\lambda}(x_{i},v), and then claim 3 of Properties of Finite Sums, gives

λ(a∗a)=βλ(a,a)=∑i=1mξi∑j=1mξjβλ(xi,xj)=∑i=1m∑j=1mξiξj mij(λ).\lambda(a^{*}a)=\beta_{\lambda}(a,a)=\sum_{i=1}^{m}\xi_{i}\sum_{j=1}^{m}\xi_{j}\beta_{\lambda}(x_{i},x_{j})=\sum_{i=1}^{m}\sum_{j=1}^{m}\xi_{i}\xi_{j}\,\mathrm{m}_{ij}(\lambda).

The left side is nonnegative by condition (b) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state.

Now let i,k∈[n]i,k\in[n], and write ai=aiT=ci1+uia_{i}=a^{T}_{i}=c_{i}1+u_{i} with ui=∑j=1mAijxju_{i}=\sum_{j=1}^{m}A_{ij}x_{j}. By (H), σT(xi)=ai\sigma_{T}(x_{i})=a_{i} and σT(xixk)=aiak\sigma_{T}(x_{i}x_{k})=a_{i}a_{k}. Linearity of λ\lambda, claim 4 of Properties of Finite Sums of Vectors and λ(1)=1\lambda(1)=1 give λ(ui)=∑jAijmj(λ)\lambda(u_{i})=\sum_{j}A_{ij}\mathrm{m}_{j}(\lambda), and therefore mi(λ∘σT)=λ(ai)=ci+∑j=1mAijmj(λ)\mathrm{m}_{i}(\lambda\circ\sigma_{T})=\lambda(a_{i})=c_{i}+\sum_{j=1}^{m}A_{ij}\mathrm{m}_{j}(\lambda). By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra and Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §monomials, aiak=cick1+ciuk+ckui+uiuka_{i}a_{k}=c_{i}c_{k}1+c_{i}u_{k}+c_{k}u_{i}+u_{i}u_{k}. By (L) and claim 4 of Properties of Finite Sums of Vectors, applied first to q↦λ(quk)q\mapsto\lambda(qu_{k}) and then to q↦λ(xjq)q\mapsto\lambda(x_{j}q), and then claim 3 of Properties of Finite Sums,

λ(uiuk)=∑j=1mAijλ(xjuk)=∑j=1mAij∑l=1mAklλ(xjxl)=∑j=1m∑l=1mAijAkl mjl(λ).\lambda(u_{i}u_{k})=\sum_{j=1}^{m}A_{ij}\lambda(x_{j}u_{k})=\sum_{j=1}^{m}A_{ij}\sum_{l=1}^{m}A_{kl}\lambda(x_{j}x_{l})=\sum_{j=1}^{m}\sum_{l=1}^{m}A_{ij}A_{kl}\,\mathrm{m}_{jl}(\lambda).

Applying λ\lambda to the expansion of aiaka_{i}a_{k} and inserting λ(uk)\lambda(u_{k}), λ(ui)\lambda(u_{i}) and λ(uiuk)\lambda(u_{i}u_{k}) gives the stated formula for mik(λ∘σT)\mathrm{m}_{ik}(\lambda\circ\sigma_{T}).

Proof of clause 4 (Coordinate data). Let i∈[d]i\in[d]. By Affine Data and Affine Substitutions of Noncommutative Polynomials §tuple, aipr1=0⋅1+∑j=12dPij1xja^{\mathrm{pr}^{1}}_{i}=0\cdot1+\sum_{j=1}^{2d}P^{1}_{ij}x_{j}, where the summands with j≠ij\neq i are 00 and the summand with j=ij=i is xix_{i}. So aipr1=xia^{\mathrm{pr}^{1}}_{i}=x_{i} by claim 7 of Properties of Finite Sums of Vectors; likewise aipr2=xd+ia^{\mathrm{pr}^{2}}_{i}=x_{d+i}. Hence σpr1=σ(x1,…,xd)=ι1\sigma_{\mathrm{pr}^{1}}=\sigma_{(x_{1},\dots,x_{d})}=\iota^{1} and σpr2=σ(xd+1,…,x2d)=ι2\sigma_{\mathrm{pr}^{2}}=\sigma_{(x_{d+1},\dots,x_{2d})}=\iota^{2} by Couplings of Two Noncommutative Laws and Their Quadratic Cost §marginals.

For i,j∈[d]i,j\in[d], the value QijQ_{ij} is 11 exactly when j=ij=i, because i=d+ji=d+j is impossible since i≤d<d+ji\le d<d+j. Likewise Qd+i,jQ_{d+i,j} is 11 exactly when j=ij=i, because d+i=jd+i=j is impossible since j≤d<d+ij\le d<d+i. So claim 7 of Properties of Finite Sums of Vectors gives aidiag=ad+idiag=xia^{\mathrm{diag}}_{i}=a^{\mathrm{diag}}_{d+i}=x_{i}, and σdiag\sigma_{\mathrm{diag}} is the substitution of (x1,…,xd,x1,…,xd)(x_{1},\dots,x_{d},x_{1},\dots,x_{d}). The same description, together with claim 7 of Properties of Finite Sums, gives for i,l∈[d]i,l\in[d]

(P1Q)il=∑k=12dPik1Qkl=Qil=Eil,(P2Q)il=∑k=12dPik2Qkl=Qd+i,l=Eil,(P^{1}Q)_{il}=\sum_{k=1}^{2d}P^{1}_{ik}Q_{kl}=Q_{il}=E_{il},\qquad(P^{2}Q)_{il}=\sum_{k=1}^{2d}P^{2}_{ik}Q_{kl}=Q_{d+i,l}=E_{il},

and hence, by claims 2 and 3 of Properties of Finite Sums, ((P1−P2)Q)il=(P1Q)il−(P2Q)il=0((P^{1}-P^{2})Q)_{il}=(P^{1}Q)_{il}-(P^{2}Q)_{il}=0. In each composite of Affine Data and Affine Substitutions of Noncommutative Polynomials §composite with diag\mathrm{diag} the second component is i↦0+∑kPik⋅0=0i\mapsto0+\sum_{k}P_{ik}\cdot0=0. Hence pr1∘diag=pr2∘diag=(E,0)=idd\mathrm{pr}^{1}\circ\mathrm{diag}=\mathrm{pr}^{2}\circ\mathrm{diag}=(E,0)=\mathrm{id}_{d}, and both maps of D∘diagD\circ\mathrm{diag} have value 00.

Let γ\gamma be a tracial state on P2d\mathcal{P}_{2d}. By claims 2, 3 and 7 of Properties of Finite Sums of Vectors, aiD=∑jPij1xj−∑jPij2xj=xi−xd+ia^{D}_{i}=\sum_{j}P^{1}_{ij}x_{j}-\sum_{j}P^{2}_{ij}x_{j}=x_{i}-x_{d+i}. Hence (H) gives σD(xj2)=(xj−xd+j)2\sigma_{D}(x_{j}^{2})=(x_{j}-x_{d+j})^{2} for j∈[d]j\in[d]. By clause 1, γ∘σD\gamma\circ\sigma_{D} is a tracial state on Pd\mathcal{P}_{d}. By claim 4 of Properties of Finite Sums of Vectors for γ\gamma and Couplings of Two Noncommutative Laws and Their Quadratic Cost §cost,

M(γ∘σD)=∑j=1dγ((xj−xd+j)2)=γ(Δd).M(\gamma\circ\sigma_{D})=\sum_{j=1}^{d}\gamma\bigl((x_{j}-x_{d+j})^{2}\bigr)=\gamma(\Delta_{d}).

By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra, (xj−xd+j)2=xj2−xjxd+j−xd+jxj+xd+j2(x_{j}-x_{d+j})^{2}=x_{j}^{2}-x_{j}x_{d+j}-x_{d+j}x_{j}+x_{d+j}^{2}. By condition (c) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state, γ(xd+jxj)=γ(xjxd+j)\gamma(x_{d+j}x_{j})=\gamma(x_{j}x_{d+j}), so γ((xj−xd+j)2)=γ(xj2)+γ(xd+j2)−2 mj,d+j(γ)\gamma((x_{j}-x_{d+j})^{2})=\gamma(x_{j}^{2})+\gamma(x_{d+j}^{2})-2\,\mathrm{m}_{j,d+j}(\gamma). Applying (H) to ι1=σpr1\iota^{1}=\sigma_{\mathrm{pr}^{1}} and ι2=σpr2\iota^{2}=\sigma_{\mathrm{pr}^{2}} gives ι1(xj2)=xj2\iota^{1}(x_{j}^{2})=x_{j}^{2} and ι2(xj2)=xd+j2\iota^{2}(x_{j}^{2})=x_{d+j}^{2}. Hence ∑jγ(xj2)=M(γ∘ι1)\sum_{j}\gamma(x_{j}^{2})=M(\gamma\circ\iota^{1}) and ∑jγ(xd+j2)=M(γ∘ι2)\sum_{j}\gamma(x_{d+j}^{2})=M(\gamma\circ\iota^{2}), where γ∘ι1\gamma\circ\iota^{1} and γ∘ι2\gamma\circ\iota^{2} are tracial states by clause 1. Summing over jj with claims 2 and 3 of Properties of Finite Sums gives γ(Δd)=M(γ∘ι1)+M(γ∘ι2)−2∑j=1dmj,d+j(γ)\gamma(\Delta_{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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