TheoremBase

Linearity, the norm bound and the vacuum formula follow from the properties of the conjugation and its right action. For dependence on the law, both vectors are approximated by universal polynomials in the resolvent transform, so each commutator norm becomes an iterated limit of numbers determined by the common law of the transforms.

Proof

Each result cited below is universally quantified over the data in its own statement.

Claims 2 to 4 are proved for an arbitrary tracial W*-probability space (H,M,Ω)(H,M,\Omega) with conjugation JJ; they therefore also hold for (K,N,Ψ)(K,N,\Psi) with JNJ_{N}. Elements of MM lie in L(H)\mathcal{L}(H) by Cyclic Tracial Operator Algebras and Their Traces §triple, and MM contains II and is closed under sums, scalar multiples, composites and adjoints, by Cyclic Tracial Operator Algebras and Their Traces §star-algebra; also ∥Ω∥=1\lVert\Omega\rVert=1 by Cyclic Tracial Operator Algebras and Their Traces §cyclic. For T∈L(H)T\in\mathcal{L}(H) and v∈Hv\in H we use ∥Tv∥≤∥T∥op∥v∥\lVert Tv\rVert\le\lVert T\rVert_{\mathrm{op}}\lVert v\rVert, which holds because ∥T∥op\lVert T\rVert_{\mathrm{op}} is a bound for TT 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, and the triangle inequality of the norm from The Induced Norm is a Norm, and Induces a Metric.

Claim 2 (Linearity). By Conjugation of a Complex Hilbert Space §conjugation, JJ is additive with J(cξ)=c‾JξJ(c\xi)=\overline{c}J\xi. Since aa is linear,

JaJ(ζ+cη)=J(aJζ+c‾ aJη)=JaJζ+c JaJη,JaJ(\zeta+c\eta)=J\bigl(aJ\zeta+\overline{c}\,aJ\eta\bigr)=JaJ\zeta+c\,JaJ\eta ,

so JaJJaJ is linear, and subtracting a(ζ+cη)=aζ+caηa(\zeta+c\eta)=a\zeta+ca\eta gives [ζ+cη,a]=[ζ,a]+c[η,a][\zeta+c\eta,a]=[\zeta,a]+c[\eta,a].

Claim 3 (Bound). By the same clause of Conjugation of a Complex Hilbert Space §conjugation, ∥Jξ∥2=⟨Jξ,Jξ⟩=⟨ξ,ξ⟩=∥ξ∥2\lVert J\xi\rVert^{2}=\langle J\xi,J\xi\rangle=\langle\xi,\xi\rangle=\lVert\xi\rVert^{2} for every ξ∈H\xi\in H. Hence ∥JaJζ∥=∥aJζ∥≤∥a∥op∥Jζ∥=∥a∥op∥ζ∥\lVert JaJ\zeta\rVert=\lVert aJ\zeta\rVert\le\lVert a\rVert_{\mathrm{op}}\lVert J\zeta\rVert=\lVert a\rVert_{\mathrm{op}}\lVert\zeta\rVert and ∥aζ∥≤∥a∥op∥ζ∥\lVert a\zeta\rVert\le\lVert a\rVert_{\mathrm{op}}\lVert\zeta\rVert, and the triangle inequality gives ∥[ζ,a]∥≤2∥a∥op∥ζ∥\lVert[\zeta,a]\rVert\le2\lVert a\rVert_{\mathrm{op}}\lVert\zeta\rVert.

Claim 4 (Vacuum vectors). By The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §right-action with S=aS=a and T=bT=b, JaJ(bΩ)=ba∗Ω=baΩJaJ(b\Omega)=ba^{*}\Omega=ba\Omega, as a∗=aa^{*}=a. So [bΩ,a]=baΩ−abΩ=(ba−ab)Ω[b\Omega,a]=ba\Omega-ab\Omega=(ba-ab)\Omega.

Claim 5 (Dependence on the law). Put Z=(sΩ,P)Z=(s\Omega,P) and Z′=(tΨ,Q)Z'=(t\Psi,Q), L2L^{2} 2d2d-tuples with Zj=sjΩZ_{j}=s_{j}\Omega and Zd+j=PjZ_{d+j}=P_{j} for j∈[d]j\in[d], and likewise for Z′Z'. Let r=R(Z)r=\mathbf{R}(Z) and r′=R(Z′)r'=\mathbf{R}(Z') be the resolvent transforms. By The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §consistent, rr is a self-adjoint 4d4d-tuple in MM and r′r' one in NN, all entries of operator norm at most 11. By The Law of the Resolvent Transform is a Lipschitz Function of the Law, and Reconstruction of a Square-Integrable Tuple from a Bounded Tuple with the Law of Its Transform §law, the hypothesis law(Z)=law(Z′)\mathrm{law}(Z)=\mathrm{law}(Z') gives λr=λr′\lambda_{r}=\lambda_{r'}. Comparing the formulas of The Resolvent of a Self-Adjoint Vector and the Resolvent Transform of a Square-Integrable Tuple §transform for the tuple ZZ and for the 11-tuple (Zk)(Z_{k}), (r2k−1,r2k)=R(Zk)(r_{2k-1},r_{2k})=\mathbf{R}(Z_{k}) for every k∈[2d]k\in[2d], and likewise in NN.

Fix a sequence (qn)(q_{n}) in P2,sa\mathcal{P}_{2,\mathrm{sa}} as in The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §recovery (named (Pn)(P_{n}) there). For k∈[2d]k\in[2d] let ek=(x2k−1,x2k)e_{k}=(x_{2k-1},x_{2k}), a 22-tuple in P4d\mathcal{P}_{4d}, and let σek:P2→P4d\sigma_{e_{k}}:\mathcal{P}_{2}\to\mathcal{P}_{4d} be its substitution. For j∈[d]j\in[d] and n,m∈Nn,m\in\mathbb{N} put Aj,n=σed+j(qn)A_{j,n}=\sigma_{e_{d+j}}(q_{n}), Bj,m=σej(qm)B_{j,m}=\sigma_{e_{j}}(q_{m}) and

Gj,n,m=Aj,nBj,m−Bj,mAj,n∈P4d;G_{j,n,m}=A_{j,n}B_{j,m}-B_{j,m}A_{j,n}\in\mathcal{P}_{4d};

these polynomials do not depend on the spaces. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §substitution and Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, Aj,n(r)=qn(r2d+2j−1,r2d+2j)=qn(R(Pj))=:pj,nA_{j,n}(r)=q_{n}(r_{2d+2j-1},r_{2d+2j})=q_{n}(\mathbf{R}(P_{j}))=:p_{j,n} and Bj,m(r)=qm(R(sjΩ))=:cj,mB_{j,m}(r)=q_{m}(\mathbf{R}(s_{j}\Omega))=:c_{j,m}. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §transport, applied to the set MM and the inclusion map of MM into L(H)\mathcal{L}(H), both lie in MM. By linearity of evaluation and Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism, Gj,n,m(r)=pj,ncj,m−cj,mpj,nG_{j,n,m}(r)=p_{j,n}c_{j,m}-c_{j,m}p_{j,n}. The same holds in NN with r′r', pj,n′=qn(R(Qj))p'_{j,n}=q_{n}(\mathbf{R}(Q_{j})) and cj,m′=qm(R(tjΨ))c'_{j,m}=q_{m}(\mathbf{R}(t_{j}\Psi)).

Fix j∈[d]j\in[d].

Step (i). Pj∈HsaP_{j}\in H_{\mathrm{sa}} by Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples, and sjΩ∈Hsas_{j}\Omega\in H_{\mathrm{sa}} by Standard Form of a Tracial W*-Probability Space: the Commutation Theorem, Right-Bounded Vectors, Faithfulness and Self-Adjoint Vectors §self-adjoint; so by The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §recovery, pj,nΩ→Pjp_{j,n}\Omega\to P_{j} as n→∞n\to\infty and cj,mΩ→sjΩc_{j,m}\Omega\to s_{j}\Omega as m→∞m\to\infty. By Claims 2 and 3 and the triangle inequality,

∣∥[Pj,sj]∥−∥[pj,nΩ,sj]∥∣≤∥[Pj−pj,nΩ,sj]∥≤2∥sj∥op∥Pj−pj,nΩ∥→0,\bigl|\lVert[P_{j},s_{j}]\rVert-\lVert[p_{j,n}\Omega,s_{j}]\rVert\bigr|\le\lVert[P_{j}-p_{j,n}\Omega,s_{j}]\rVert\le2\lVert s_{j}\rVert_{\mathrm{op}}\lVert P_{j}-p_{j,n}\Omega\rVert\to0 ,

so ∥[Pj,sj]∥=lim⁡n∥[pj,nΩ,sj]∥\lVert[P_{j},s_{j}]\rVert=\lim_{n}\lVert[p_{j,n}\Omega,s_{j}]\rVert.

Step (ii). Fix nn and write p=pj,np=p_{j,n}, c=cj,mc=c_{j,m}. By Claim 4, [pΩ,sj]=(psj−sjp)Ω[p\Omega,s_{j}]=(ps_{j}-s_{j}p)\Omega, and

(psj−sjp)Ω−(pc−cp)Ω=p(sj−c)Ω−(sj−c)pΩ.(ps_{j}-s_{j}p)\Omega-(pc-cp)\Omega=p(s_{j}-c)\Omega-(s_{j}-c)p\Omega .

Since p,sj−c∈Mp,s_{j}-c\in M, the two inequalities of Resolvents in a Tracial W*-Probability Space: Product Bounds, Membership, the L^2 Lipschitz Bound, and Extension to Self-Adjoint Vectors §products bound the norm of the right side by 2∥p∥op∥sjΩ−cΩ∥2\lVert p\rVert_{\mathrm{op}}\lVert s_{j}\Omega-c\Omega\rVert, which tends to 00 as m→∞m\to\infty by Step (i). Hence ∥[pj,nΩ,sj]∥=lim⁡m∥Gj,n,m(r)Ω∥\lVert[p_{j,n}\Omega,s_{j}]\rVert=\lim_{m}\lVert G_{j,n,m}(r)\Omega\rVert.

Step (iii). By The Law of a Tuple of Bounded Self-Adjoint Operators in a Tracial Vector State §state, applied with the tuple rr, bound 11 and the unit vector Ω\Omega, and since its map λT\lambda_{T} is then the law λr\lambda_{r}, we get ∥G(r)Ω∥2=λr(G∗G)\lVert G(r)\Omega\rVert^{2}=\lambda_{r}(G^{*}G) for every G∈P4dG\in\mathcal{P}_{4d}, and likewise ∥G(r′)Ψ∥2=λr′(G∗G)\lVert G(r')\Psi\rVert^{2}=\lambda_{r'}(G^{*}G). As λr=λr′\lambda_{r}=\lambda_{r'} and norms are nonnegative, gj,n,m:=∥Gj,n,m(r)Ω∥=∥Gj,n,m(r′)Ψ∥g_{j,n,m}:=\lVert G_{j,n,m}(r)\Omega\rVert=\lVert G_{j,n,m}(r')\Psi\rVert.

Step (iv). Steps (i) and (ii), with the order of limits: first m→∞m\to\infty for each fixed nn, then n→∞n\to\infty, give ∥[Pj,sj]∥=lim⁡nlim⁡mgj,n,m\lVert[P_{j},s_{j}]\rVert=\lim_{n}\lim_{m}g_{j,n,m}. The same steps in (K,N,Ψ)(K,N,\Psi), using that QjQ_{j} and tjΨt_{j}\Psi are fixed by JNJ_{N} by the same two results, give ∥[Qj,tj]∥=lim⁡nlim⁡mgj,n,m\lVert[Q_{j},t_{j}]\rVert=\lim_{n}\lim_{m}g_{j,n,m} with the same numbers gj,n,mg_{j,n,m}. Hence ∥[Pj,sj]∥=∥[Qj,tj]∥\lVert[P_{j},s_{j}]\rVert=\lVert[Q_{j},t_{j}]\rVert for every j∈[d]j\in[d], and summing the squares over jj proves the claim.

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