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Proof of The Law of a Tuple of Bounded Self-Adjoint Operators in a Tracial Vector State

lemmalem:nc-law-operator-tuple-2026a
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· 6,262 chars · 13 deps · depth 21 Reason: G5: proof that a tracial operator tuple has a law in Sigma_{n,R}.

The state properties follow from the homomorphism and adjoint properties of evaluation, Cauchy-Schwarz and the word-product norm bound, and traciality extends from pairs of monomials to all pairs of polynomials by the uniqueness of linear extension from monomials, applied once in each argument.

Proof

Each result cited below is universally quantified over the data in its own statement. We work in the setting of Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation and Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation. Fix nn, RR, HH, Ω\Omega and TT as in the statement. By Complex Hilbert Spaces and Bounded Linear Maps: Standing Notation §maps, sums and scalar multiples in L(H)\mathcal{L}(H) are formed pointwise, so (A+B)Ω=AΩ+BΩ(A+B)\Omega=A\Omega+B\Omega and (aA)Ω=a (AΩ)(aA)\Omega=a\,(A\Omega) for A,B∈L(H)A,B\in\mathcal{L}(H) and a∈Ca\in\mathbb{C}. By Complex Hilbert Space, HH is a complex inner product space; its inner product is additive and homogeneous in the second argument by conditions 2 and 3 of Complex Inner Product Space.

Step 1 (linearity and normalisation). Let p,q∈Pnp,q\in\mathcal{P}_{n} and a∈Ca\in\mathbb{C}. The evaluation p↦p(T)p\mapsto p(T) is linear by Evaluation of Noncommutative Polynomials at a Tuple of Bounded Operators §evaluation, so (p+q)(T)=p(T)+q(T)(p+q)(T)=p(T)+q(T) and (ap)(T)=a p(T)(ap)(T)=a\,p(T). Hence, by the pointwise operations and conditions 2 and 3 of Complex Inner Product Space,

λT(p+q)=⟨Ω,p(T)Ω+q(T)Ω⟩=λT(p)+λT(q),λT(ap)=⟨Ω,a (p(T)Ω)⟩=a λT(p),\lambda_{T}(p+q)=\langle\Omega,p(T)\Omega+q(T)\Omega\rangle=\lambda_{T}(p)+\lambda_{T}(q),\qquad\lambda_{T}(ap)=\langle\Omega,a\,(p(T)\Omega)\rangle=a\,\lambda_{T}(p),

so λT\lambda_{T} is linear in the sense of Linear Map, C\mathbb{C} being a complex vector space over itself. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, 1(T)=I1(T)=I, so by Norm Induced by a Complex Inner Product and ∥Ω∥=1\lVert\Omega\rVert=1,

λT(1)=⟨Ω,Ω⟩=∥Ω∥2=1.\lambda_{T}(1)=\langle\Omega,\Omega\rangle=\lVert\Omega\rVert^{2}=1.

Step 2 (positivity). Let p∈Pnp\in\mathcal{P}_{n}. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism applied to p∗p^{*} and pp, (p∗p)(T)=p∗(T) p(T)(p^{*}p)(T)=p^{*}(T)\,p(T), and since every TjT_{j} is self-adjoint, p∗(T)=p(T)∗p^{*}(T)=p(T)^{*} by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §adjoint. As p(T)∈L(H)p(T)\in\mathcal{L}(H) and HH is a complex Hilbert space, p(T)p(T) has an adjoint 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, 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 gives

λT(p∗p)=⟨Ω,p(T)∗p(T)Ω⟩=∥p(T)Ω∥2.\lambda_{T}(p^{*}p)=\langle\Omega,p(T)^{*}p(T)\Omega\rangle=\lVert p(T)\Omega\rVert^{2}.

By Norm Induced by a Complex Inner Product this number equals ⟨p(T)Ω,p(T)Ω⟩\langle p(T)\Omega,p(T)\Omega\rangle, which is a real number with 0≤⟨p(T)Ω,p(T)Ω⟩0\le\langle p(T)\Omega,p(T)\Omega\rangle by condition 4 of Complex Inner Product Space.

Step 3 (norm bound). Let k∈Nk\in\mathbb{N} and let w∈Wnw\in W_{n} be a word of length kk. By Evaluation of Noncommutative Polynomials at a Tuple of Bounded Operators §evaluation, xw(T)=Twx_{w}(T)=T_{w}, so λT(xw)=⟨Ω,TwΩ⟩\lambda_{T}(x_{w})=\langle\Omega,T_{w}\Omega\rangle. By claim 1 of The Induced Norm is a Norm, and Induces a Metric and ∥Ω∥=1\lVert\Omega\rVert=1,

∣λT(xw)∣≤∥Ω∥ ∥TwΩ∥=∥TwΩ∥.|\lambda_{T}(x_{w})|\le\lVert\Omega\rVert\,\lVert T_{w}\Omega\rVert=\lVert T_{w}\Omega\rVert.

The operator TwT_{w} lies in L(H)\mathcal{L}(H) by Evaluation of Noncommutative Polynomials at a Tuple of Bounded Operators §word-products; 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, ∥Tw∥op\lVert T_{w}\rVert_{\mathrm{op}} is a bound for TwT_{w}, so by Bounded Linear Maps between Complex Normed Spaces and the Operator Norm §bounded we have ∥TwΩ∥≤∥Tw∥op∥Ω∥=∥Tw∥op\lVert T_{w}\Omega\rVert\le\lVert T_{w}\rVert_{\mathrm{op}}\lVert\Omega\rVert=\lVert T_{w}\rVert_{\mathrm{op}}. Since ∥Tj∥op≤R\lVert T_{j}\rVert_{\mathrm{op}}\le R for every j∈[n]j\in[n], Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §bound gives ∥Tw∥op≤Rk\lVert T_{w}\rVert_{\mathrm{op}}\le R^{k}. By transitivity of ≤\le in the ordered field R\mathbb{R}, ∣λT(xw)∣≤Rk|\lambda_{T}(x_{w})|\le R^{k}. Steps 1 to 3 prove Clause 1.

Step 4 (traciality on pairs of monomials). Assume from now on that ⟨Ω,TuTvΩ⟩=⟨Ω,TvTuΩ⟩\langle\Omega,T_{u}T_{v}\Omega\rangle=\langle\Omega,T_{v}T_{u}\Omega\rangle for all u,v∈Wnu,v\in W_{n}. Let u,v∈Wnu,v\in W_{n}. By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §monomials, xuxv=xuvx_{u}x_{v}=x_{uv}; by Evaluation of Noncommutative Polynomials at a Tuple of Bounded Operators §evaluation and Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, (xuv)(T)=Tuv=TuTv(x_{uv})(T)=T_{uv}=T_{u}T_{v}. Hence λT(xuxv)=⟨Ω,TuTvΩ⟩\lambda_{T}(x_{u}x_{v})=\langle\Omega,T_{u}T_{v}\Omega\rangle, and in the same way λT(xvxu)=⟨Ω,TvTuΩ⟩\lambda_{T}(x_{v}x_{u})=\langle\Omega,T_{v}T_{u}\Omega\rangle. By the assumption,

λT(xuxv)=λT(xvxu)for all u,v∈Wn.\lambda_{T}(x_{u}x_{v})=\lambda_{T}(x_{v}x_{u})\qquad\text{for all }u,v\in W_{n}.

Step 5 (one monomial factor). Fix v∈Wnv\in W_{n} and define f,g:Pn→Cf,g:\mathcal{P}_{n}\to\mathbb{C} by f(p)=λT(p xv)f(p)=\lambda_{T}(p\,x_{v}) and g(p)=λT(xv p)g(p)=\lambda_{T}(x_{v}\,p). By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra, for p,q∈Pnp,q\in\mathcal{P}_{n} and a∈Ca\in\mathbb{C} we have (p+q)xv=pxv+qxv(p+q)x_{v}=px_{v}+qx_{v}, (ap)xv=a(pxv)(ap)x_{v}=a(px_{v}), xv(p+q)=xvp+xvqx_{v}(p+q)=x_{v}p+x_{v}q and xv(ap)=a(xvp)x_{v}(ap)=a(x_{v}p); together with the linearity of λT\lambda_{T} from Step 1, ff and gg are linear. By Step 4, f(xu)=g(xu)f(x_{u})=g(x_{u}) for every u∈Wnu\in W_{n}. Let c:Wn→Cc:W_{n}\to\mathbb{C} be the map c(u)=f(xu)c(u)=f(x_{u}). Then ff and gg are linear maps Pn→C\mathcal{P}_{n}\to\mathbb{C} with value c(u)c(u) at xux_{u} for every uu, so f=gf=g by the uniqueness in part (a) of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §linear-extension. Thus λT(p xv)=λT(xv p)\lambda_{T}(p\,x_{v})=\lambda_{T}(x_{v}\,p) for all p∈Pnp\in\mathcal{P}_{n} and v∈Wnv\in W_{n}.

Step 6 (traciality). Fix p∈Pnp\in\mathcal{P}_{n} and define F,G:Pn→CF,G:\mathcal{P}_{n}\to\mathbb{C} by F(q)=λT(pq)F(q)=\lambda_{T}(pq) and G(q)=λT(qp)G(q)=\lambda_{T}(qp). By Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §algebra, p(q+r)=pq+prp(q+r)=pq+pr, p(aq)=a(pq)p(aq)=a(pq), (q+r)p=qp+rp(q+r)p=qp+rp and (aq)p=a(qp)(aq)p=a(qp) for q,r∈Pnq,r\in\mathcal{P}_{n} and a∈Ca\in\mathbb{C}, so FF and GG are linear by Step 1. By Step 5, F(xv)=λT(p xv)=λT(xv p)=G(xv)F(x_{v})=\lambda_{T}(p\,x_{v})=\lambda_{T}(x_{v}\,p)=G(x_{v}) for every v∈Wnv\in W_{n}, so F=GF=G by the uniqueness in part (a) of Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §linear-extension, applied as in Step 5 to the map v↦F(xv)v\mapsto F(x_{v}). Hence λT(pq)=λT(qp)\lambda_{T}(pq)=\lambda_{T}(qp) for all p,q∈Pnp,q\in\mathcal{P}_{n}.

Step 7 (conclusion). By Steps 1, 2 and 6, λT\lambda_{T} is a linear map Pn→C\mathcal{P}_{n}\to\mathbb{C} satisfying conditions (a), (b) and (c) of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §tracial-state (with d=nd=n), so it is a tracial state on Pn\mathcal{P}_{n}. By Step 3 it has norm bound RR in the sense of Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §norm-bound. Therefore λT∈Σn,R\lambda_{T}\in\Sigma_{n,R}, the set named in Noncommutative Laws, Couplings and the Wasserstein Distance: Standing Notation §laws, which proves Clause 2.

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