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Proof of The Tracial W*-Closure of a Cyclic Tracial Operator Algebra: the Commutant of the Right Action is a Tracial W*-Probability Space Equal to the Double Commutant

theoremthm:tracial-w-star-closure-2026a
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· 9,587 chars · 10 deps · depth 16 Reason: V-A1: proof of the W*-closure theorem.

M=(JAJ)' contains A because the right action JAJ commutes with A; a right-bounded vector defines a bounded operator on the dense subspace A-Omega commuting with JAJ; the relation J(T Omega)=T* Omega is checked against the dense set A-Omega and gives traciality; M'=JMJ follows from right-boundedness and separation; and M=A'' because JA'J lies in M.

Proof

Each result cited below is universally quantified over the data in its own statement. We prove the claims in the order 1 (containment), 3 (right-bounded vectors), 2 (tracial W*-probability space), 4 (commutant), 5 (double commutant); each uses only the claims proved before it.

Preliminaries. By The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §conjugation, JJ is a conjugation of HH in the sense of Conjugation of a Complex Hilbert Space §conjugation, with J(SΩ)=S∗ΩJ(S\Omega)=S^{*}\Omega for S∈AS\in\mathcal{A} and JΩ=ΩJ\Omega=\Omega. By Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §conjugation, JAJ∈L(H)JAJ\in\mathcal{L}(H) for every A∈L(H)A\in\mathcal{L}(H), so JAJ⊆L(H)J\mathcal{A}J\subseteq\mathcal{L}(H) and M=(JAJ)′M=(J\mathcal{A}J)' is defined; that clause also gives (JAJ)∗=JA∗J(JAJ)^{*}=JA^{*}J, (JAJ)(JBJ)=J(AB)J(JAJ)(JBJ)=J(AB)J, J(JAJ)J=AJ(JAJ)J=A, J(A+B)J=JAJ+JBJJ(A+B)J=JAJ+JBJ and J(cA)J=c‾ JAJJ(cA)J=\overline{c}\,JAJ for A,B∈L(H)A,B\in\mathcal{L}(H) and c∈Cc\in\mathbb{C}, which we use without further mention. Since ∥Jξ∥2=⟨Jξ,Jξ⟩=⟨ξ,ξ⟩\lVert J\xi\rVert^{2}=\langle J\xi,J\xi\rangle=\langle\xi,\xi\rangle, JJ preserves norms, and Jξ−Jη=J(ξ−η)J\xi-J\eta=J(\xi-\eta) by additivity. By The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §right-action, for all S,U∈AS,U\in\mathcal{A},

JSJ∈A′,JSJ(UΩ)=US∗Ω,in particularJSJΩ=S∗Ω  (U=I).JSJ\in\mathcal{A}',\qquad JSJ(U\Omega)=US^{*}\Omega,\qquad\text{in particular}\qquad JSJ\Omega=S^{*}\Omega\ \ (U=I).

Two consequences. (P1) JAJJ\mathcal{A}J is closed under adjoints: (JSJ)∗=JS∗J(JSJ)^{*}=JS^{*}J with S∗∈AS^{*}\in\mathcal{A} by Cyclic Tracial Operator Algebras and Their Traces §star-algebra. (P2) JAJΩ=AΩJ\mathcal{A}J\Omega=\mathcal{A}\Omega: JSJΩ=S∗Ω∈AΩJSJ\Omega=S^{*}\Omega\in\mathcal{A}\Omega, and conversely SΩ=(S∗)∗Ω=JS∗JΩS\Omega=(S^{*})^{*}\Omega=J S^{*}J\Omega with S∗∈AS^{*}\in\mathcal{A}, using (S∗)∗=S(S^{*})^{*}=S from 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. Let D=AΩD=\mathcal{A}\Omega. By Cyclic Tracial Operator Algebras and Their Traces §star-algebra, DD is a linear subspace (SΩ+cUΩ=(S+cU)ΩS\Omega+cU\Omega=(S+cU)\Omega and 0=(0⋅I)Ω0=(0\cdot I)\Omega), and by Cyclic Tracial Operator Algebras and Their Traces §cyclic it is dense in HH. (P3) A vector v∈Hv\in H with ⟨η,v⟩=0\langle\eta,v\rangle=0 for every η∈D\eta\in D is zero: for every η∈D\eta\in D, ∥v∥2=⟨v−η,v⟩+⟨η,v⟩=⟨v−η,v⟩≤∥v−η∥ ∥v∥\lVert v\rVert^{2}=\langle v-\eta,v\rangle+\langle\eta,v\rangle=\langle v-\eta,v\rangle\le\lVert v-\eta\rVert\,\lVert v\rVert by Cauchy-Schwarz Inequality in a Complex Inner Product Space, and ∥v−η∥\lVert v-\eta\rVert can be made smaller than any real ε>0\varepsilon>0 by density of DD; so ∥v∥2≤ε∥v∥\lVert v\rVert^{2}\le\varepsilon\lVert v\rVert for every ε>0\varepsilon>0, which forces ∥v∥=0\lVert v\rVert=0, i.e. v=0v=0.

Claim 1. Let S∈AS\in\mathcal{A}. For every U∈AU\in\mathcal{A} we have JUJ∈A′JUJ\in\mathcal{A}', so S(JUJ)=(JUJ)SS(JUJ)=(JUJ)S. Thus S∈L(H)S\in\mathcal{L}(H) commutes with every element of JAJJ\mathcal{A}J, i.e. S∈(JAJ)′=MS\in(J\mathcal{A}J)'=M by The Commutant of a Set of Bounded Operators on a Complex Hilbert Space §commutant. Hence A⊆M\mathcal{A}\subseteq M. By Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §order, JAJ⊆(JAJ)′′=((JAJ)′)′=M′J\mathcal{A}J\subseteq(J\mathcal{A}J)''=\bigl((J\mathcal{A}J)'\bigr)'=M'.

Claim 3. Let ζ\zeta and CC be as in the claim. Define T0:D→HT_{0}:D\to H by T0(SΩ)=JS∗JζT_{0}(S\Omega)=JS^{*}J\zeta for S∈AS\in\mathcal{A}. It is well defined: if S,S′∈AS,S'\in\mathcal{A} with SΩ=S′ΩS\Omega=S'\Omega, put R=S−S′∈AR=S-S'\in\mathcal{A}, so RΩ=0R\Omega=0 and R∗=S∗−S′∗R^{*}=S^{*}-S'^{*} 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-calculus; then R∗∈AR^{*}\in\mathcal{A} and, by the hypothesis applied to R∗R^{*} and by The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §trace,

∥JS∗Jζ−JS′∗Jζ∥=∥JR∗Jζ∥≤C∥R∗Ω∥=C∥RΩ∥=0.\lVert JS^{*}J\zeta-JS'^{*}J\zeta\rVert=\lVert JR^{*}J\zeta\rVert\le C\lVert R^{*}\Omega\rVert=C\lVert R\Omega\rVert=0.

It is linear: for S,U∈AS,U\in\mathcal{A} and c∈Cc\in\mathbb{C}, (S+cU)∗=S∗+c‾ U∗(S+cU)^{*}=S^{*}+\overline{c}\,U^{*} 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-calculus, so T0(SΩ+cUΩ)=J(S∗+c‾ U∗)Jζ=JS∗Jζ+c JU∗Jζ=T0(SΩ)+c T0(UΩ)T_{0}(S\Omega+cU\Omega)=J(S^{*}+\overline{c}\,U^{*})J\zeta=JS^{*}J\zeta+c\,JU^{*}J\zeta=T_{0}(S\Omega)+c\,T_{0}(U\Omega). It is bounded by CC: ∥T0(SΩ)∥=∥JS∗Jζ∥≤C∥S∗Ω∥=C∥SΩ∥\lVert T_{0}(S\Omega)\rVert=\lVert JS^{*}J\zeta\rVert\le C\lVert S^{*}\Omega\rVert=C\lVert S\Omega\rVert, again by the hypothesis (for S∗∈AS^{*}\in\mathcal{A}) and The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §trace. By Bounded Linear and Conjugate-Linear Maps on a Dense Subspace of a Complex Hilbert Space Extend Uniquely §linear there is T∈L(H)T\in\mathcal{L}(H) extending T0T_{0} with ∥T∥op≤C\lVert T\rVert_{\mathrm{op}}\le C. Since I∗=II^{*}=I 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-calculus, and JIJξ=J(Jξ)=ξJIJ\xi=J(J\xi)=\xi, we get TΩ=T0(IΩ)=JIJζ=ζT\Omega=T_{0}(I\Omega)=JIJ\zeta=\zeta.

T∈MT\in M: let U∈AU\in\mathcal{A}. For S∈AS\in\mathcal{A}, JUJ(SΩ)=SU∗ΩJUJ(S\Omega)=SU^{*}\Omega with SU∗∈ASU^{*}\in\mathcal{A}, and (SU∗)∗=US∗(SU^{*})^{*}=US^{*} 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-calculus, so

T JUJ SΩ=T0(SU∗Ω)=J(US∗)Jζ=(JUJ)(JS∗J)ζ=JUJ TSΩ.T\,JUJ\,S\Omega=T_{0}(SU^{*}\Omega)=J(US^{*})J\zeta=(JUJ)(JS^{*}J)\zeta=JUJ\,T S\Omega.

The operators T JUJT\,JUJ and JUJ TJUJ\,T in L(H)\mathcal{L}(H) agree on DD, so they are equal by Bounded Linear and Conjugate-Linear Maps on a Dense Subspace of a Complex Hilbert Space Extend Uniquely §equality. Hence TT commutes with JAJJ\mathcal{A}J, i.e. T∈MT\in M.

Uniqueness: let T,T′∈MT,T'\in M with TΩ=T′Ω=ζT\Omega=T'\Omega=\zeta. Then R=T−T′∈MR=T-T'\in M by Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §algebra and RΩ=0R\Omega=0. For S∈AS\in\mathcal{A}, R(JSJΩ)=JSJ(RΩ)=0R(JSJ\Omega)=JSJ(R\Omega)=0, so RR vanishes on JAJΩ=DJ\mathcal{A}J\Omega=D (P2), and R=0R=0 by Bounded Linear and Conjugate-Linear Maps on a Dense Subspace of a Complex Hilbert Space Extend Uniquely §equality.

Claim 2. We check the three conditions of Cyclic Tracial Operator Algebras and Their Traces §triple for (H,M,Ω)(H,M,\Omega). Condition (a): by Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §algebra applied to S=JAJ\mathcal{S}=J\mathcal{A}J, I∈MI\in M and MM is closed under sums, scalar multiples and products; by (P1), (JAJ)∗⊆JAJ(J\mathcal{A}J)^{*}\subseteq J\mathcal{A}J, so the same clause gives T∗∈MT^{*}\in M for T∈MT\in M. Condition (b): ∥Ω∥=1\lVert\Omega\rVert=1 by Cyclic Tracial Operator Algebras and Their Traces §cyclic for A\mathcal{A}, and MΩ⊇AΩ=DM\Omega\supseteq\mathcal{A}\Omega=D by Claim 1, so MΩM\Omega is dense, since every open ball of HH meets DD.

Next, J(TΩ)=T∗ΩJ(T\Omega)=T^{*}\Omega for every T∈MT\in M. Let S∈AS\in\mathcal{A}. Using ⟨Jξ,Jη⟩=⟨η,ξ⟩\langle J\xi,J\eta\rangle=\langle\eta,\xi\rangle and JJξ=ξJJ\xi=\xi, then S∗Ω=JSJΩS^{*}\Omega=JSJ\Omega, then (JSJ)∗=JS∗J(JSJ)^{*}=JS^{*}J, then T(JS∗J)=(JS∗J)TT(JS^{*}J)=(JS^{*}J)T (as T∈MT\in M) and JS∗JΩ=(S∗)∗Ω=SΩJS^{*}J\Omega=(S^{*})^{*}\Omega=S\Omega; the two steps that move an operator across the inner product are the adjoint relation, by Adjoint of a Linear Map between Complex Inner Product Spaces §adjoint (in the last step applied to T∗T^{*}, whose adjoint is 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 §adjoint-calculus):

⟨SΩ,JTΩ⟩=⟨JJTΩ,JSΩ⟩=⟨TΩ,S∗Ω⟩=⟨TΩ,JSJΩ⟩=⟨JS∗J TΩ,Ω⟩=⟨T JS∗JΩ,Ω⟩=⟨TSΩ,Ω⟩=⟨SΩ,T∗Ω⟩.\langle S\Omega,JT\Omega\rangle=\langle JJT\Omega,JS\Omega\rangle=\langle T\Omega,S^{*}\Omega\rangle=\langle T\Omega,JSJ\Omega\rangle=\langle JS^{*}J\,T\Omega,\Omega\rangle=\langle T\,JS^{*}J\Omega,\Omega\rangle=\langle TS\Omega,\Omega\rangle=\langle S\Omega,T^{*}\Omega\rangle .

So v=JTΩ−T∗Ωv=JT\Omega-T^{*}\Omega satisfies ⟨η,v⟩=0\langle\eta,v\rangle=0 for all η∈D\eta\in D, and v=0v=0 by (P3).

Condition (c): for S,T∈MS,T\in M, using the adjoint relation (by Adjoint of a Linear Map between Complex Inner Product Spaces §adjoint), J(SΩ)=S∗ΩJ(S\Omega)=S^{*}\Omega, J(TΩ)=T∗ΩJ(T\Omega)=T^{*}\Omega and ⟨Jξ,Jη⟩=⟨η,ξ⟩\langle J\xi,J\eta\rangle=\langle\eta,\xi\rangle with ξ=SΩ\xi=S\Omega, η=JTΩ\eta=JT\Omega,

⟨Ω,STΩ⟩=⟨S∗Ω,TΩ⟩=⟨JSΩ,TΩ⟩,⟨Ω,TSΩ⟩=⟨T∗Ω,SΩ⟩=⟨JTΩ,SΩ⟩=⟨JSΩ,JJTΩ⟩=⟨JSΩ,TΩ⟩.\langle\Omega,ST\Omega\rangle=\langle S^{*}\Omega,T\Omega\rangle=\langle JS\Omega,T\Omega\rangle,\qquad\langle\Omega,TS\Omega\rangle=\langle T^{*}\Omega,S\Omega\rangle=\langle JT\Omega,S\Omega\rangle=\langle JS\Omega,JJT\Omega\rangle=\langle JS\Omega,T\Omega\rangle.

So (H,M,Ω)(H,M,\Omega) is a cyclic tracial operator algebra. By Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §order, M′′=(JAJ)′′′=(JAJ)′=MM''=(J\mathcal{A}J)'''=(J\mathcal{A}J)'=M, so (H,M,Ω)(H,M,\Omega) is a tracial W*-probability space by Tracial W*-Probability Spaces §space. Its trace is τM(T)=⟨Ω,TΩ⟩\tau_{M}(T)=\langle\Omega,T\Omega\rangle by Tracial W*-Probability Spaces §trace and Cyclic Tracial Operator Algebras and Their Traces §trace, which equals τA(T)\tau_{\mathcal{A}}(T) for T∈A⊆MT\in\mathcal{A}\subseteq M. Finally JJ is a conjugation of HH with J(TΩ)=T∗ΩJ(T\Omega)=T^{*}\Omega for every T∈MT\in M, so by the uniqueness in The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §conjugation, applied to (H,M,Ω)(H,M,\Omega), JJ is the conjugation of (H,M,Ω)(H,M,\Omega).

Claim 4. First JMJ⊆M′JMJ\subseteq M': for T∈MT\in M, The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §right-action applied to the cyclic tracial operator algebra (H,M,Ω)(H,M,\Omega), whose conjugation is JJ by Claim 2, gives JTJ∈M′JTJ\in M'. Conversely let y∈M′y\in M' and put ζ=JyΩ\zeta=Jy\Omega. For S∈AS\in\mathcal{A} we have S∈MS\in M by Claim 1, so Sy=ySSy=yS, and

∥JSJζ∥=∥JSJJyΩ∥=∥JSyΩ∥=∥SyΩ∥=∥ySΩ∥≤∥y∥op∥SΩ∥\lVert JSJ\zeta\rVert=\lVert JSJJy\Omega\rVert=\lVert JSy\Omega\rVert=\lVert Sy\Omega\rVert=\lVert yS\Omega\rVert\le\lVert y\rVert_{\mathrm{op}}\lVert S\Omega\rVert

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. By Claim 3 with C=∥y∥opC=\lVert y\rVert_{\mathrm{op}} there is T∈MT\in M with TΩ=JyΩT\Omega=Jy\Omega. Then JTJ∈M′JTJ\in M', and JTJΩ=JTΩ=JJyΩ=yΩJTJ\Omega=JT\Omega=JJy\Omega=y\Omega since JΩ=ΩJ\Omega=\Omega. Thus JTJ−y∈M′JTJ-y\in M' (by Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §algebra) vanishes at Ω\Omega, and The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §separating, applied to (H,M,Ω)(H,M,\Omega), gives y=JTJ∈JMJy=JTJ\in JMJ. Hence M′=JMJM'=JMJ.

Claim 5. Since A⊆M\mathcal{A}\subseteq M (Claim 1), two applications of Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §order give M′⊆A′M'\subseteq\mathcal{A}' and A′′⊆M′′=M\mathcal{A}''\subseteq M''=M (Claim 2). Conversely let y∈A′y\in\mathcal{A}'. Then JyJ∈L(H)JyJ\in\mathcal{L}(H) and, for S∈AS\in\mathcal{A}, (JyJ)(JSJ)=J(yS)J=J(Sy)J=(JSJ)(JyJ)(JyJ)(JSJ)=J(yS)J=J(Sy)J=(JSJ)(JyJ), so JyJ∈(JAJ)′=MJyJ\in(J\mathcal{A}J)'=M. Hence y=J(JyJ)J∈JMJ=M′y=J(JyJ)J\in JMJ=M' by Claim 4. So A′⊆M′\mathcal{A}'\subseteq M', and Basic Properties of Commutants: Unital Algebras Closed under Weak Limits, Order Reversal, the Triple Commutant, and Conjugation §order gives M=M′′⊆A′′M=M''\subseteq\mathcal{A}''. Therefore M=A′′M=\mathcal{A}''.

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