TheoremBase

Uniqueness comes from the separating property of the vacuum. For existence, polynomials in the resolvent transform that approximate the reference operators LxjL_{x_j} uniformly give right-bounded approximants of XjX_j, so the standard-form theorem yields sjs_j; its law is lambda because kappadkappa_d is injective.

Proof

Each result cited below is universally quantified over the data in its own statement. Recall that (H,M,Ω)(H,M,\Omega) is a cyclic tracial operator algebra with M=M′′M=M'' by Tracial W*-Probability Spaces §space, so I∈MI\in M and MM is closed under sums, complex multiples, composition and adjoints by Cyclic Tracial Operator Algebras and Their Traces §star-algebra, and ∥Ω∥=1\lVert\Omega\rVert=1 by Cyclic Tracial Operator Algebras and Their Traces §cyclic; hence p(T)∈Mp(T)\in M for every p∈Pnp\in\mathcal{P}_{n} and every nn-tuple TT in MM, by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §transport applied with A=M\mathcal{A}=M and Φ\Phi the identity map. Evaluation p↦p(T)p\mapsto p(T) is linear by Evaluation of Noncommutative Polynomials at a Tuple of Bounded Operators §evaluation.

Step 1 (Uniqueness). If s,s′s,s' are self-adjoint dd-tuples in MM with sΩ=s′Ω=Xs\Omega=s'\Omega=X, then for each j∈[d]j\in[d] we have sj−sj′∈Ms_{j}-s'_{j}\in M and (sj−sj′)Ω=0(s_{j}-s'_{j})\Omega=0, so sj=sj′s_{j}=s'_{j} by The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §separating.

For Steps 2 to 8 fix j∈[d]j\in[d].

Step 2 (Reference realisation). Since λ∈Σd,R⊆Σd\lambda\in\Sigma_{d,R}\subseteq\Sigma_{d} (the inclusion by Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §law), the triple (Hλ,Mλ,Ωλ)(\mathcal{H}_{\lambda},\mathcal{M}_{\lambda},\Omega_{\lambda}) is a tracial W*-probability space by The Tracial Algebra of a Noncommutative Law is a Tracial W*-Probability Space: the W*-Closure of the Left Multiplications §w-star. Let t=(Lx1,…,Lxd)t=(L_{x_{1}},\dots,L_{x_{d}}). Each tkt_{k} lies in Mλ\mathcal{M}_{\lambda} 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 §star-algebra, is self-adjoint by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §adjoint (as xk∗=xkx_{k}^{*}=x_{k} by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §adjoint), and satisfies ∥tk∥op≤R\lVert t_{k}\rVert_{\mathrm{op}}\le R by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §multiplication with r=Rr=R. By the definition of λt\lambda_{t} and The Tracial Algebra of a Noncommutative Law is a Tracial W*-Probability Space: the W*-Closure of the Left Multiplications §law, λt(p)=⟨Ωλ,p(t)Ωλ⟩=λ(p)\lambda_{t}(p)=\langle\Omega_{\lambda},p(t)\Omega_{\lambda}\rangle=\lambda(p) for all pp, so λt=λ\lambda_{t}=\lambda, and by Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §bounded law(tΩλ)=κd(λ)=law(X)\mathrm{law}(t\Omega_{\lambda})=\kappa_{d}(\lambda)=\mathrm{law}(X).

Step 3 (Transfer through the resolvent law). By The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §consistent, R(X)\mathbf{R}(X) is a self-adjoint 2d2d-tuple in MM with entries of operator norm at most 11, and R(tΩλ)=R(t)\mathbf{R}(t\Omega_{\lambda})=\mathbf{R}(t); 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 and Step 2, λR(X)=λR(tΩλ)=λR(t)\lambda_{\mathbf{R}(X)}=\lambda_{\mathbf{R}(t\Omega_{\lambda})}=\lambda_{\mathbf{R}(t)}. By the definition of the transforms and its operator version, R(Xj)=(R(X)2j−1,R(X)2j)\mathbf{R}(X_{j})=(\mathbf{R}(X)_{2j-1},\mathbf{R}(X)_{2j}) and R(tj)=(R(t)2j−1,R(t)2j)\mathbf{R}(t_{j})=(\mathbf{R}(t)_{2j-1},\mathbf{R}(t)_{2j}). Let a=(x2j−1,x2j)a=(x_{2j-1},x_{2j}), a 22-tuple in P2d\mathcal{P}_{2d}. For every 2d2d-tuple TT of operators, a(T)=(T2j−1,T2j)a(T)=(T_{2j-1},T_{2j}) by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, so, where σa:P2→P2d\sigma_{a}:\mathcal{P}_{2}\to\mathcal{P}_{2d} is the substitution of aa, σa(r)(T)=r(T2j−1,T2j)\sigma_{a}(r)(T)=r(T_{2j-1},T_{2j}) for r∈P2r\in\mathcal{P}_{2} by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §substitution. Evaluating the equal laws at σa(r)\sigma_{a}(r) gives, for every r∈P2r\in\mathcal{P}_{2},

(∗)⟨Ω,r(R(Xj))Ω⟩=⟨Ωλ,r(R(tj))Ωλ⟩.(\ast)\qquad\langle\Omega,r(\mathbf{R}(X_{j}))\Omega\rangle=\langle\Omega_{\lambda},r(\mathbf{R}(t_{j}))\Omega_{\lambda}\rangle.

Step 4 (Uniform polynomials). Let n∈Nn\in\mathbb{N}. First choose y=1+2nR3y=1+2nR^{3}, so y≥1y\ge1 and R3/y2≤1/(2n)R^{3}/y^{2}\le1/(2n); then put ε=1/(2ny2)\varepsilon=1/(2ny^{2}); then take p∈P2p\in\mathcal{P}_{2} from Calculus of Resolvents of Bounded Self-Adjoint Operators: Adjoints, Commutation, the Resolvent Identity, Recovery, Stepping, and Uniform Polynomial Approximation §transform for s=ys=y and ε\varepsilon; finally set qn=y22(p+p∗)q_{n}=\tfrac{y^{2}}{2}(p+p^{*}), which lies in P2,sa\mathcal{P}_{2,\mathrm{sa}} by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §self-adjoint. Let KK be a complex Hilbert space and A∈L(K)A\in\mathcal{L}(K) self-adjoint with ∥A∥op≤R\lVert A\rVert_{\mathrm{op}}\le R. Put E=Ry(A)−p(R(A))E=R_{y}(A)-p(\mathbf{R}(A)), so ∥E∥op≤ε\lVert E\rVert_{\mathrm{op}}\le\varepsilon. The entries of R(A)\mathbf{R}(A) are self-adjoint by Calculus of Resolvents of Bounded Self-Adjoint Operators: Adjoints, Commutation, the Resolvent Identity, Recovery, Stepping, and Uniform Polynomial Approximation §parts, so p(R(A))∗=p∗(R(A))p(\mathbf{R}(A))^{*}=p^{*}(\mathbf{R}(A)) by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §adjoint; with Ry(A)∗=R−y(A)R_{y}(A)^{*}=R_{-y}(A) from Calculus of Resolvents of Bounded Self-Adjoint Operators: Adjoints, Commutation, the Resolvent Identity, Recovery, Stepping, and Uniform Polynomial Approximation §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, E∗=R−y(A)−p∗(R(A))E^{*}=R_{-y}(A)-p^{*}(\mathbf{R}(A)), and ∥E∗∥op=∥E∥op\lVert E^{*}\rVert_{\mathrm{op}}=\lVert E\rVert_{\mathrm{op}} 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. Hence

A−qn(R(A))=(A−y22(Ry(A)+R−y(A)))+y22(E+E∗),A-q_{n}(\mathbf{R}(A))=\Bigl(A-\tfrac{y^{2}}{2}\bigl(R_{y}(A)+R_{-y}(A)\bigr)\Bigr)+\tfrac{y^{2}}{2}(E+E^{*}),

and by Calculus of Resolvents of Bounded Self-Adjoint Operators: Adjoints, Commutation, the Resolvent Identity, Recovery, Stepping, and Uniform Polynomial Approximation §recovery and the norm rules 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, ∥A−qn(R(A))∥op≤R3/y2+y2ε≤1/n\lVert A-q_{n}(\mathbf{R}(A))\rVert_{\mathrm{op}}\le R^{3}/y^{2}+y^{2}\varepsilon\le1/n. The polynomial qnq_{n} depends only on nn and RR.

Step 5 (Approximants and their moments). Let bn=qn(R(Xj))∈Mb_{n}=q_{n}(\mathbf{R}(X_{j}))\in M and cn=qn(R(tj))∈L(Hλ)c_{n}=q_{n}(\mathbf{R}(t_{j}))\in\mathcal{L}(\mathcal{H}_{\lambda}); both are self-adjoint by Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §adjoint, as R(Xj)\mathbf{R}(X_{j}) and R(tj)\mathbf{R}(t_{j}) have self-adjoint entries (Step 3 and The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §consistent). By Step 4 with A=tjA=t_{j}, ∥cn−tj∥op≤1/n\lVert c_{n}-t_{j}\rVert_{\mathrm{op}}\le1/n, so ∥cn∥op≤R+1/n\lVert c_{n}\rVert_{\mathrm{op}}\le R+1/n. For m∈Nm\in\mathbb{N}, applying (∗)(\ast) to the product rr of 2m2m factors qnq_{n} and using Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism, ⟨Ω,bn2mΩ⟩=⟨Ωλ,cn2mΩλ⟩\langle\Omega,b_{n}^{2m}\Omega\rangle=\langle\Omega_{\lambda},c_{n}^{2m}\Omega_{\lambda}\rangle; since cn2mc_{n}^{2m} is the value of the monomial x12m∈P1x_{1}^{2m}\in\mathcal{P}_{1} at the 11-tuple (cn)(c_{n}) (Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values, Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism) and ∥Ωλ∥=1\lVert\Omega_{\lambda}\rVert=1 by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §vacuum, The Law of a Tuple of Bounded Self-Adjoint Operators in a Tracial Vector State §state gives ∣⟨Ω,bn2mΩ⟩∣≤(R+1/n)2m|\langle\Omega,b_{n}^{2m}\Omega\rangle|\le(R+1/n)^{2m}.

Step 6 (A moment bound gives a right multiplication bound). Let b∈Mb\in M be self-adjoint and C>0C>0 real with ∣⟨Ω,b2mΩ⟩∣≤C2m|\langle\Omega,b^{2m}\Omega\rangle|\le C^{2m} for all m∈Nm\in\mathbb{N}; we show ∥bTΩ∥≤C∥TΩ∥\lVert bT\Omega\rVert\le C\lVert T\Omega\rVert for every T∈MT\in M. Put u1=12(T+T∗)u_{1}=\tfrac12(T+T^{*}) and u2=12i(T−T∗)u_{2}=\tfrac{1}{2i}(T-T^{*}); they lie in MM, are self-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-calculus, and T=u1+iu2T=u_{1}+iu_{2}. Let V=(b,u1,u2)V=(b,u_{1},u_{2}) and ν=λV\nu=\lambda_{V}; then, with R′=1+∥b∥op+∥u1∥op+∥u2∥opR'=1+\lVert b\rVert_{\mathrm{op}}+\lVert u_{1}\rVert_{\mathrm{op}}+\lVert u_{2}\rVert_{\mathrm{op}}, ν∈Σ3\nu\in\Sigma_{3} by Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §law applied with the bound R′R', so ν\nu is a tracial state (Noncommutative Laws of Finitely Many Self-Adjoint Variables with a Norm Bound §law). By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §values and Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism, together with the linearity of evaluation, x12m(V)=b2mx_{1}^{2m}(V)=b^{2m}, (x2+ix3)(V)=T(x_{2}+ix_{3})(V)=T and (x1(x2+ix3))(V)=bT(x_{1}(x_{2}+ix_{3}))(V)=bT. The number ν(x12m)=⟨Ω,b2mΩ⟩\nu(x_{1}^{2m})=\langle\Omega,b^{2m}\Omega\rangle is real (as noted 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 §multiplication), so ν(x12m)≤C2m\nu(x_{1}^{2m})\le C^{2m}, and 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 §multiplication with a=x1a=x_{1} (x1∈P3,sax_{1}\in\mathcal{P}_{3,\mathrm{sa}} by Noncommutative Polynomials Form a Unital Complex Algebra with Involution: Linear Extension from Monomials, Products, Adjoints and Self-Adjoint Parts §self-adjoint), S=CS=C and p=x2+ix3p=x_{2}+ix_{3} gives ∥x1p∥ν≤C∥p∥ν\lVert x_{1}p\rVert_{\nu}\le C\lVert p\rVert_{\nu}. By The Law of a Tuple of Bounded Self-Adjoint Operators in a Tracial Vector State §state (with bound R′R'), ∥q∥ν=∥q(V)Ω∥\lVert q\rVert_{\nu}=\lVert q(V)\Omega\rVert for every q∈P3q\in\mathcal{P}_{3}, whence ∥bTΩ∥≤C∥TΩ∥\lVert bT\Omega\rVert\le C\lVert T\Omega\rVert. Applied to b=bnb=b_{n}, C=R+1/nC=R+1/n (Step 5) and T=S∗T=S^{*}, and using ∥S∗Ω∥=∥SΩ∥\lVert S^{*}\Omega\rVert=\lVert S\Omega\rVert from The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §trace: ∥bnS∗Ω∥≤(R+1/n)∥SΩ∥\lVert b_{n}S^{*}\Omega\rVert\le(R+1/n)\lVert S\Omega\rVert for every S∈MS\in M.

Step 7 (bnΩ→Xjb_{n}\Omega\to X_{j}). Take (Pm)(P_{m}) from The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §recovery and put D=qn−PmD=q_{n}-P_{m}. By Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §homomorphism and Evaluation of Noncommutative Polynomials at Bounded Operators: a Unital Homomorphism Compatible with Adjoints, Substitution, Representations and the GNS Multiplication Operators §adjoint, (D∗D)(R(Xj))=D(R(Xj))∗D(R(Xj))(D^{*}D)(\mathbf{R}(X_{j}))=D(\mathbf{R}(X_{j}))^{*}D(\mathbf{R}(X_{j})), and likewise at R(tj)\mathbf{R}(t_{j}); so (∗)(\ast) with r=D∗Dr=D^{*}D and the identity ⟨v,T∗Tv⟩=∥Tv∥2\langle v,T^{*}Tv\rangle=\lVert Tv\rVert^{2} 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 give

∥bnΩ−Pm(R(Xj))Ω∥=∥cnΩλ−Pm(R(tj))Ωλ∥.\lVert b_{n}\Omega-P_{m}(\mathbf{R}(X_{j}))\Omega\rVert=\lVert c_{n}\Omega_{\lambda}-P_{m}(\mathbf{R}(t_{j}))\Omega_{\lambda}\rVert .

Now XjX_{j} is fixed by JJ (Square-Integrable Tuples in a Tracial W*-Probability Space: Their Norm, Affine Images, Pairs, Embedded Images and Laws §tuples) and tjΩλt_{j}\Omega_{\lambda} is fixed by the conjugation of (Hλ,Mλ,Ωλ)(\mathcal{H}_{\lambda},\mathcal{M}_{\lambda},\Omega_{\lambda}) (Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §law); and R(tjΩλ)=R(tj)\mathbf{R}(t_{j}\Omega_{\lambda})=\mathbf{R}(t_{j}) by The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §consistent. So, as m→∞m\to\infty, Pm(R(Xj))Ω→XjP_{m}(\mathbf{R}(X_{j}))\Omega\to X_{j} and Pm(R(tj))Ωλ→tjΩλP_{m}(\mathbf{R}(t_{j}))\Omega_{\lambda}\to t_{j}\Omega_{\lambda} by The Resolvent Transform of Square-Integrable Tuples: Consistency, Concatenation, the L^2 Lipschitz Bound and Universal Polynomial Recovery §recovery, and continuity of the norm gives ∥bnΩ−Xj∥=∥(cn−tj)Ωλ∥≤∥cn−tj∥op≤1/n\lVert b_{n}\Omega-X_{j}\rVert=\lVert(c_{n}-t_{j})\Omega_{\lambda}\rVert\le\lVert c_{n}-t_{j}\rVert_{\mathrm{op}}\le1/n 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 Step 5.

Step 8 (The operator sjs_{j}). Let S∈MS\in M. By The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §right-action, JSJ∈M′⊆L(H)JSJ\in M'\subseteq\mathcal{L}(H) and JSJ(bnΩ)=bnS∗ΩJSJ(b_{n}\Omega)=b_{n}S^{*}\Omega. As JSJJSJ is bounded, Step 7 gives JSJXj=lim⁡nbnS∗ΩJSJX_{j}=\lim_{n}b_{n}S^{*}\Omega, so by Step 6 ∥JSJXj∥≤lim⁡n(R+1/n)∥SΩ∥=R∥SΩ∥\lVert JSJX_{j}\rVert\le\lim_{n}(R+1/n)\lVert S\Omega\rVert=R\lVert S\Omega\rVert. By Standard Form of a Tracial W*-Probability Space: the Commutation Theorem, Right-Bounded Vectors, Faithfulness and Self-Adjoint Vectors §right-bounded with C=RC=R there is sj∈Ms_{j}\in M with sjΩ=Xjs_{j}\Omega=X_{j} and ∥sj∥op≤R\lVert s_{j}\rVert_{\mathrm{op}}\le R. By The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §conjugation, sj∗Ω=J(sjΩ)=JXj=Xj=sjΩs_{j}^{*}\Omega=J(s_{j}\Omega)=JX_{j}=X_{j}=s_{j}\Omega, and sj∗−sj∈Ms_{j}^{*}-s_{j}\in M, so sj∗=sjs_{j}^{*}=s_{j} by The Trace, the Conjugation and the Right Action of a Cyclic Tracial Operator Algebra §separating. Thus s=(s1,…,sd)s=(s_{1},\dots,s_{d}) is a self-adjoint dd-tuple in MM with sΩ=Xs\Omega=X; with Step 1 this proves clause 1, and the bound proves clause 2.

Step 9 (Law). By Calculus of Laws of Square-Integrable Tuples: Bounded Tuples, the Lipschitz Bound, Moments, Affine Push-Forwards, Couplings and Embeddings §bounded, κd(λs)=law(sΩ)=law(X)=κd(λ)\kappa_{d}(\lambda_{s})=\mathrm{law}(s\Omega)=\mathrm{law}(X)=\kappa_{d}(\lambda), where λs∈Σd\lambda_{s}\in\Sigma_{d} by Laws of Self-Adjoint Tuples in a Tracial W*-Probability Space: Moments, Affine Images, Couplings, Embeddings and L^2 Approximation §law. Since (Σd,W2)(\Sigma_{d},W_{2}) is a metric space by The Noncommutative Wasserstein Distance Satisfies the Triangle Inequality and is a Metric on Noncommutative Laws §metric and κd\kappa_{d} is its canonical map, κd\kappa_{d} is injective by The Metric Completion is a Complete Metric Space with a Dense Isometric Copy of the Space, and Maps Preserving Cauchy Sequences Extend to It §isometry; hence λs=λ\lambda_{s}=\lambda, which is clause 3.

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