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Ultraproduct expectations and semi-lift ambiguity

Written by GPT-6.1 Sol (OpenAI), Ultra. Course exposition: CC0-1.0 to the extent of rights held. Earlier programme and human-source notices retain their own terms.

The multiplier construction gives a von Neumann algebra Mω=Nω/IωM^\omega=N_\omega/I_\omega with a normal constant copy of MM. Taking the ultraweak limit of a representative recovers an element of MM. We construct this map, prove its normality directly, and use it to distinguish the information in a convergent automorphism family from the information in its limit.

Throughout Sections 1–2, MM has a faithful normal state φ\varphi, and ω\omega is free. Section 3 assumes separable predual when using Mω=Cω/IωM_\omega=C_\omega/I_\omega. Section 4 uses the tracial hyperfinite II1\mathrm{II}_1 factor RR. Inputs are the preceding quotient and normal embedding proofs, ultraweak compactness of bounded balls, and the already proved tensor model for RR. We construct the expectation directly from the quotient. The complete multiplier and faithful quotient-state proofs, normal-functional coefficient and bounded topology proofs, and order-normal positive-functional theorem NF1–4 supply their exact full prerequisites. The tracial Hilbert-space arguments and full dyadic tensor model supply the finite tensor example. The general centralizing algebra is constructed below without a factor assumption.

The centralizing algebra at nonfactor scope

The C* algebra and norm estimates in the first paragraphs use only a faithful normal state. The countable metric-completion argument below additionally assumes separable predual, as in Section 3. For the module convention (xψ)(a)=ψ(ax)(x\psi)(a)=\psi(ax), (ψx)(a)=ψ(xa)(\psi x)(a)=\psi(xa), let CωC_\omega be the bounded sequences whose commutators with every fixed ψ∈M∗\psi\in M_* tend to zero along ω\omega. The identity [ab,ψ]=a[b,ψ]+[a,ψ]b[ab,\psi]=a[b,\psi]+[a,\psi]b, the corresponding adjoint identity obtained by conjugating functionals, and ∥[a,ψ]∥≤2∥a∥∥ψ∥\|[a,\psi]\|\le2\|a\|\|\psi\| show that this is a norm-closed unital C* algebra.

Every bounded strong*-null sequence belongs to CωC_\omega. For a vector-pair functional, its two module products are bounded by the norm of the fixed vector times the norm of the null operator or its adjoint on the other fixed vector. Every normal functional is a summable vector-pair series; a finite head and the uniform operator bound control its tail. This proves the assertion for all normal functionals, also along an ultrafilter.

For completeness Cω⊂NωC_\omega\subset N_\omega. If ∥an∥≤C\|a_n\|\le C, ∥bn∥≤K\|b_n\|\le K, aa is centralizing and b∈Iωb\in I_\omega, moving an∗a_n^* past the state and then applying Cauchy–Schwarz gives

φ(an∗bn∗bnan)≤∣φ(bn∗bnanan∗)∣+CK2∥[an∗,φ]∥≤C2K φ(bn∗bn)1/2+CK2∥[an∗,φ]∥⟶ω0. \begin{aligned} \varphi(a_n^*b_n^*b_na_n) &\le |\varphi(b_n^*b_na_na_n^*)| +CK^2\|[a_n^*,\varphi]\|\\ &\le C^2K\,\varphi(b_n^*b_n)^{1/2} +CK^2\|[a_n^*,\varphi]\|\longrightarrow_\omega0. \end{aligned}

Indeed φ((bn∗bn)2)≤K2φ(bn∗bn)\varphi((b_n^*b_n)^2)\le K^2\varphi(b_n^*b_n) and φ((anan∗)2)≤C4\varphi((a_na_n^*)^2)\le C^4. The adjoint estimate uses bnbn∗b_nb_n^* and [an,φ][a_n,\varphi]. The two other product seminorms are directly at most CC times the corresponding seminorm of bnb_n. Thus both multiplier conditions hold. Hence IωI_\omega is a closed two-sided ideal in CωC_\omega, and Cω/IωC_\omega/I_\omega embeds isometrically into MωM^\omega.

The restricted faithful quotient state λ=φω\lambda=\varphi^\omega is a trace, since for centralizing representatives

∣φ(anbn−bnan)∣≤sup⁡n∥bn∥ ∥[an,φ]∥⟶ω0. |\varphi(a_nb_n-b_na_n)| \le \sup_n\|b_n\|\,\|[a_n,\varphi]\|\longrightarrow_\omega0.

Its squared trace norm is exactly the ultralimit of the squared symmetric seminorm. This trace depends on the chosen center state in general; no scalar trace invariant under every automorphism of a nonfactor is asserted.

Here is the full metric-completion step. Now assume separable predual. For a Cauchy sequence of quotient contractions choose a subsequence ArA_r with ∥Ar−Ap∥2,λ<2−p\|A_r-A_p\|_{2,\lambda}<2^{-p} for r>pr>p. Continuous radial clipping gives centralizing contraction lifts ar(k)a_r(k). Choose a norm-dense countable family ψj\psi_j in M∗M_*, and nested sets Wr∈ωW_r\in\omega, each contained in {k:k≥r}\{k:k\ge r\}, on which

∥[ar(k),ψj]∥<1/r(j≤r),∥ar(k)−ap(k)∥φ,#<2−p+2−r(p<r). \begin{aligned} \|[a_r(k),\psi_j]\|&<1/r &&(j\le r),\\ \|a_r(k)-a_p(k)\|_{\varphi,\#} &<2^{-p}+2^{-r} &&(p<r). \end{aligned}

Each step intersects only finitely many large sets. Put r(k)=max⁡{r≤k:k∈Wr}r(k)=\max\{r\le k:k\in W_r\}, or zero when empty, and a(k)=ar(k)(k)a(k)=a_{r(k)}(k), with a0=0a_0=0. For every fixed rr, the set WrW_r forces r(k)≥rr(k)\ge r, so r(k)→ω∞r(k)\to_\omega\infty. The commutator tests and the uniform contraction bound imply a∈Cωa\in C_\omega by norm density. For fixed pp, the second line yields ∥π(a)−Ap∥2,λ≤2−p\|\pi(a)-A_p\|_{2,\lambda}\le2^{-p}. Thus the subsequence, and then the whole Cauchy sequence, converges in the quotient unit ball.

This metric completeness also handles an arbitrary Cauchy net in that ball: choose successively indices whose tails have diameters below 2−r2^{-r}, making the indices increasing by directedness. The selected sequence is Cauchy and has a limit; its tail-diameter bounds force the original net to that same limit. No cofinal sequence of the net is asserted.

Apply bounded strong* density to the C* subalgebra Cω/IωC_\omega/I_\omega in the faithful normal representation of MωM^\omega. A bounded approximating net for an element of its von Neumann closure is Cauchy for ∥⋅∥2,λ\|\cdot\|_{2,\lambda}; the complete metric ball gives its limit in the quotient itself. Traciality makes both symmetric state seminorms converge. The bounded faithful-state topology then makes this the strong* limit in MωM^\omega, so it is the original approximated element. Consequently the subalgebra is strongly closed. Its inclusion is normal because all its vector-pair coefficients, and their summable series, are restrictions of those on MωM^\omega. The restriction of the faithful normal state is a faithful normal trace. A proper isometry would have positive range defect of zero trace, contradicting faithfulness; hence the algebra is finite. This proves all the needed structural assertions for MωM_\omega, with arbitrary center.

1. The canonical ultraweak-limit map

Theorem 1.1. The formula

Eω(π(xn))=uw-lim⁡n→ωxn(1)E_\omega(\pi(x_n))=\operatorname*{uw-lim}_{n\to\omega}x_n \tag{1}

defines a faithful normal unital completely positive MM-bimodule map Eω:Mω→ME_\omega:M^\omega\to M. It fixes the constant copy of MM, and

φ∘Eω=φω.(2)\varphi\circ E_\omega=\varphi^\omega. \tag{2}

In particular it is an expectation onto that copy.

Proof. A bounded sequence has a unique ultraweak ultralimit, since a bounded closed ball of MM is compact Hausdorff for that topology. A sequence in IωI_\omega converges strong* to zero along ω\omega, hence ultraweakly to zero. Thus (1) is independent of the representative.

It is linear, unital and fixes constants. For a,b∈Ma,b\in M, their constant sequences are multipliers, and separate ultraweak continuity of multiplication gives

Eω(aXb)=aEω(X)b.(3)E_\omega(aXb)=aE_\omega(X)b. \tag{3}

Complete positivity can be checked at every finite matrix level. A positive element of Mk(Mω)M_k(M^\omega) has a positive lift in Mk(Nω)M_k(N_\omega): lift its positive square root and multiply the lift by its adjoint. Every coordinate matrix is positive. Its entrywise ultraweak limit is positive because the positive cone of Mk(M)M_k(M) is ultraweakly closed. These entries are exactly the values of the matrix amplification of (1).

Equation (2) follows from the definition of the quotient state. To prove normality, let 0≤Xi↑X0\le X_i\uparrow X be an arbitrary bounded increasing net in MωM^\omega, and put Y=sup⁡iEω(Xi)Y=\sup_i E_\omega(X_i) in MM. Positivity gives Y≤Eω(X)Y\le E_\omega(X). Normality of the two states and (2) give

φ(Eω(X)−Y)=φω(X)−lim⁡iφω(Xi)=0.(4)\varphi(E_\omega(X)-Y) =\varphi^\omega(X)-\lim_i\varphi^\omega(X_i)=0. \tag{4}

The positive difference vanishes by faithfulness of φ\varphi. Thus EωE_\omega preserves increasing positive suprema and is normal. If X≥0X\ge0 and Eω(X)=0E_\omega(X)=0, then φω(X)=0\varphi^\omega(X)=0; the faithful quotient state makes X=0X=0. This proves faithfulness as well. To verify full ultraweak continuity, compose EωE_\omega with each positive normal functional ρ\rho of MM. Preservation of increasing positive suprema makes ρEω\rho E_\omega order-normal, so the complete theorem NF1–4 places it in (Mω)∗(M^\omega)_*. Every normal functional is a linear combination of four positive normal functionals. Thus all predual coefficients pull back to actual predual coefficients, which is exactly ultraweak continuity on the whole domain. □\square

The map depends on the ultrafilter but not on the state used to describe the strong*-null ideal. The state identity (2) is a convenient proof of normality, rather than an extra definition of the map. On each fixed norm ball the two faithful normal-state symmetric seminorms describe the same topology. Continuity at zero therefore supplies, for each positive tolerance in one seminorm, a positive tolerance in the other, uniformly over that ball. Applying this implication on an ultrafilter-large set proves equality of their null ideals. The multiplier algebra is the normalizer of that ideal and hence is unchanged. Formula (1) uses only ultraweak ultralimits in the original algebra, so it gives the same expectation after this identification.

2. Covariance of a chosen semi-lift

For a fixed normal automorphism β\beta, write βω\beta^\omega for its constant lift. If βn→β\beta_n\to\beta in the uu-topology, retain the family in

Γ(βn)(π(xn))=π(βn(xn)).(5)\Gamma_{(\beta_n)}(\pi(x_n))=\pi(\beta_n(x_n)). \tag{5}

The preceding lesson proves that this is a normal automorphism, and that its restriction to MM is β\beta. The coordinate map and its inverse preserve the null ideal, the two-sided multiplier condition and the centralizing commutator tests. Once the induced map is a *-automorphism of the von Neumann quotient, it preserves every bounded increasing positive supremum, because it and its inverse preserve order. NF1–4 applied to each positive normal coefficient then proves its full ultraweak continuity. No state-preservation assumption is needed for this normality argument.

Here is a direct proof of the coordinate-lift assertions at the general faithful-state scope. The coordinate map on bounded sequences is an isometric *-automorphism. If b=(bn)∈Iωb=(b_n)\in I_\omega and ∥bn∥≤C\|b_n\|\le C, then

φ(βn(bn)∗βn(bn))≤C2∥φ∘βn−φ∘β∥+(φ∘β)(bn∗bn)⟶ω0. \begin{aligned} \varphi(\beta_n(b_n)^*\beta_n(b_n)) &\le C^2\|\varphi\circ\beta_n-\varphi\circ\beta\| +(\varphi\circ\beta)(b_n^*b_n) \longrightarrow_\omega0. \end{aligned}

The adjoint square has the same bound with bnbn∗b_nb_n^*. The final terms tend to zero because fixed normal positive functionals test the same bounded strong* topology as the faithful state. The inverse family also converges in the uu-topology: composing with βn\beta_n, an isometry on the predual, gives

∥ψ∘βn−1−ψ∘β−1∥=∥ψ−(ψ∘β−1)∘βn∥⟶0. \|\psi\circ\beta_n^{-1}-\psi\circ\beta^{-1}\| =\|\psi-(\psi\circ\beta^{-1})\circ\beta_n\| \longrightarrow0.

Thus both coordinate maps preserve IωI_\omega. Its two-sided normalizer NωN_\omega is consequently invariant too, by applying the coordinate automorphism to both ideal-preservation equations. This yields a *-automorphism of MωM^\omega, normal by the order and coefficient argument just given.

For a fixed a∈Ma\in M, uu-convergence implies βn(a)→β(a)\beta_n(a)\to\beta(a) strong*. To check it directly after reducing the limit to the identity, expand each square of βn(a)−a\beta_n(a)-a. The first term is tested by ψ∘βn\psi\circ\beta_n at a∗aa^*a. The two cross terms are tested at a,a∗a,a^* by the fixed normal functionals x↦ψ(a∗x)x\mapsto\psi(a^*x) and x↦ψ(xa)x\mapsto\psi(xa). Their limits cancel the two diagonal terms. Repeat for the adjoint square and every positive normal ψ\psi. Hence the quotient restriction to constants is precisely β\beta.

For centralizing (an)(a_n), bounded by CC, the module identity gives

∥[βn(an),ψ]∥≤∥[an,ψ∘β]∥+2C∥ψ∘βn−ψ∘β∥⟶ω0. \|[\beta_n(a_n),\psi]\| \le \|[a_n,\psi\circ\beta]\| +2C\|\psi\circ\beta_n-\psi\circ\beta\| \longrightarrow_\omega0.

The inverse estimate proves invariance of CωC_\omega in both directions. None of these arguments uses separable predual, a factor assumption, or preservation of the chosen state. Under the separable-predual hypothesis of Section 3, the restriction is an automorphism of the finite normally embedded centralizing von Neumann algebra constructed above.

Proposition 2.1. Every such chosen family satisfies

EωΓ(βn)=βEω.(6)E_\omega\Gamma_{(\beta_n)}=\beta E_\omega. \tag{6}

Proof. If ∥xn∥≤C\|x_n\|\le C and ψ∈M∗\psi\in M_*, then

∣ψ(βn(xn))−ψ(β(xn))∣≤C∥ψ∘βn−ψ∘β∥⟶0.(7)|\psi(\beta_n(x_n))-\psi(\beta(x_n))| \le C\|\psi\circ\beta_n-\psi\circ\beta\|\longrightarrow0. \tag{7}

The ultraweak ultralimit of β(xn)\beta(x_n) is β(Eω(X))\beta(E_\omega(X)), by normality of β\beta. Taking scalar ultralimits in (7) proves (6). □\square

Consequently every convergent family with limit β\beta gives the same action on the constant algebra and the same covariance with EωE_\omega. These two conclusions do not determine its action on varying quotient elements. Nor is φω\varphi^\omega automatically preserved: its transformed state is (φ∘β)∘Eω(\varphi\circ\beta)\circ E_\omega, which equals φω\varphi^\omega when β\beta preserves φ\varphi.

3. A trace with values in the original center

Assume now that MM has separable predual, without imposing a factor hypothesis. The preceding lesson embeds the finite von Neumann algebra MωM_\omega normally in MωM^\omega.

Theorem 3.1. The restriction

Tω=Eω∣Mω:Mω→Z(M)(8)T_\omega=E_\omega|_{M_\omega}:M_\omega\to Z(M) \tag{8}

is a faithful normal unital positive trace with values in Z(M)Z(M). It fixes the constant copy of Z(M)Z(M), is a Z(M)Z(M)-bimodule map, and satisfies

Tω(XY)=Tω(YX),X,Y∈Mω.(9)T_\omega(XY)=T_\omega(YX),\qquad X,Y\in M_\omega. \tag{9}

Here the specified value algebra is the center of the original MM; no equality with Z(Mω)Z(M_\omega) is asserted.

Proof. For X=π(xn)X=\pi(x_n), centralizing means ∥[xn,ψ]∥→ω0\|[x_n,\psi]\|\to_\omega0 for every ψ∈M∗\psi\in M_*. For fixed a∈Ma\in M, this gives

∣ψ(xna−axn)∣≤∥a∥∥[xn,ψ]∥→ω0.(10)|\psi(x_na-ax_n)|\le\|a\|\|[x_n,\psi]\|\to_\omega0. \tag{10}

Passing to the ultraweak limit shows that Eω(X)E_\omega(X) commutes with every aa, so belongs to Z(M)Z(M). For centralizing representatives xn,ynx_n,y_n,

∣ψ(xnyn−ynxn)∣≤sup⁡n∥yn∥∥[xn,ψ]∥→ω0,(11)|\psi(x_ny_n-y_nx_n)| \le\sup_n\|y_n\|\|[x_n,\psi]\|\to_\omega0, \tag{11}

which proves (9) for every normal functional.

The positivity, faithfulness and normality are restrictions of Theorem 1.1. A constant central element is centralizing, since its functional commutators vanish exactly. Equations (1) and (3) therefore give the remaining assertions. □\square

If MM is a factor, the value algebra is C1\mathbb C1. Thus Tω(X)=τω(X)1T_\omega(X)=\tau_\omega(X)1, and the trace on MωM_\omega is independent of the particular faithful normal state of MM. For a nonfactor, composing (8) with a faithful normal state on Z(M)Z(M) gives its corresponding faithful normal scalar trace.

4. Two different semi-lifts with the same limit

Use the concrete tracial tensor model

R=⨂n≥1(M2,tr⁡2)‾ vN.(12)R=\overline{\bigotimes_{n\ge1}(M_2,\operatorname{tr}_2)}^{\,\mathrm{vN}}. \tag{12}

Let znz_n and xnx_n be identity on every tensor leg except leg nn, where they equal

z=(100−1),x=(0110).(13)z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}, \qquad x=\begin{pmatrix}0&1\\1&0\end{pmatrix}. \tag{13}

They are self-adjoint unitaries, with trace zero and zx=−xzzx=-xz. Each sequence commutes eventually with every finite tensor word. Approximating any a∈Ra\in R in trace 22-norm by such words proves

∥[zn,a]∥2, ∥[xn,a]∥2⟶0.(14)\|[z_n,a]\|_2,\ \|[x_n,a]\|_2\longrightarrow0. \tag{14}

The finite trace centralizing criterion from the preceding lessons makes these sequences centralizing. Equivalently, finite tensor densities are dense in L1(R,τ)L^1(R,\tau), so their commutation proves the required convergence against every normal functional.

The density assertion has a direct whole-predual proof. In the trace representation, every normal functional is a norm-convergent summable vector-pair series. Its finite head can be approximated by vector pairs aΩ,bΩa\Omega,b\Omega with a,ba,b in finite tensor stages; the coefficient error is at most ∥ξ−aΩ∥∥η∥+∥aΩ∥∥η−bΩ∥\|\xi-a\Omega\|\|\eta\|+\|a\Omega\|\|\eta-b\Omega\|. These coefficients are y↦τ(b∗ya)=τ(ab∗y)y\mapsto\tau(b^*ya)=\tau(ab^*y), so finite tensor densities are norm dense in R∗R_*. HF0's full isometric trace pairing identifies the completion for ∥h∥1=τ(∣h∣)\|h\|_1=\tau(|h|) with that entire predual. Alternatively its inequality ∥h∥1≤∥h∥2\|h\|_1\le\|h\|_2 for bounded hh, and finite-stage Hilbert density, show the same density in this completion. Thus eventual commutation with every finite tensor density, followed by the uniform commutator bound, gives centralizing against every normal functional. Adjoint conjugation is an isometry on the predual; the same dense coefficients are eventually fixed by the tail conjugations. This also proves ordinary uu-convergence used in Proposition 4.1.

Put Z=π(zn)Z=\pi(z_n), X=π(xn)X=\pi(x_n) in RωR_\omega. They satisfy

Z2=X2=1,Z∗=Z,X∗=X,ZX=−XZ.(15)Z^2=X^2=1,\qquad Z^*=Z,\quad X^*=X,\qquad ZX=-XZ. \tag{15}

Their trace 22-norms are one, so neither is zero.

Proposition 4.1. The families βn=Ad⁡(zn)\beta_n=\operatorname{Ad}(z_n) and β~n=id\widetilde\beta_n=\mathrm{id} both converge to id\mathrm{id} in the uu-topology, but induce different normal automorphisms of RωR^\omega, even on RωR_\omega.

Proof. The ordinary centralizing unitary criterion gives Ad⁡(zn)→id\operatorname{Ad}(z_n)\to\mathrm{id} in the uu-topology. It can also be checked directly on the dense finite tensor normal functionals: they are eventually fixed, and conjugation is an isometry on the predual. The induced automorphisms are

Γ(βn)=Ad⁡(Z),Γ(β~n)=id.(16)\Gamma_{(\beta_n)}=\operatorname{Ad}(Z),\qquad \Gamma_{(\widetilde\beta_n)}=\mathrm{id}. \tag{16}

By (15), the first sends XX to −X-X, whereas the second fixes XX. Their difference on XX has trace 22-norm two. Both restrict to the identity on constant RR and obey EωΓ=EωE_\omega\Gamma=E_\omega. □\square

A prescribed constant restriction therefore does not determine the automorphism on varying quotient elements. What is proved for each chosen family is a normal automorphism with that constant restriction and the covariance (6). The family cannot be suppressed from the notation merely because it converges.

5. Two limits on a fast reindexing theorem

The same example prevents fast reindexing with unrestricted semi-lift equivariance.

Proposition 5.1. There are separable von Neumann subalgebras P,Q⊂RωP,Q\subset R^\omega and a countable group GG of semi-liftable automorphisms preserving PP, for which no injective *-homomorphism can satisfy simultaneously

Φ(P∩Rω)⊂Q′∩Rω,γΦ=Φγ(γ∈G).(17)\Phi(P\cap R_\omega)\subset Q'\cap R_\omega, \qquad \gamma\Phi=\Phi\gamma\quad(\gamma\in G). \tag{17}

Proof. Take P=Q=W∗(X,Z)P=Q=W^*(X,Z), and G={id,γ}G=\{\mathrm{id},\gamma\}, with γ=Ad⁡(Z)\gamma=\operatorname{Ad}(Z). Relations (15) give P≅M2P\cong M_2: the projections (1±Z)/2(1\pm Z)/2, and their off-diagonal operators obtained from XX, are matrix units. Both projections have trace 1/21/2, so the representation is faithful. In particular PP has separable predual and lies in RωR_\omega. The group has order two, is semi-liftable by (16), and preserves PP.

The first condition of (17) makes Φ(X)\Phi(X) commute with ZZ, hence γ(Φ(X))=Φ(X)\gamma(\Phi(X))=\Phi(X). Equivariance and γ(X)=−X\gamma(X)=-X instead give γ(Φ(X))=−Φ(X)\gamma(\Phi(X))=-\Phi(X). Thus Φ(X)=0\Phi(X)=0, contradicting injectivity. □\square

There is also a separate obstruction to full scalar trace independence when constants are fixed. Let a=xa=x be a constant trace-zero self-adjoint unitary in M2⊂RM_2\subset R, and let P,QP,Q contain it. Then

τω(aΦ(x))=τ(a2)=1,τω(a)τω(x)=0(18)\tau^\omega(a\Phi(x))=\tau(a^2)=1, \qquad \tau^\omega(a)\tau^\omega(x)=0 \tag{18}

for every map fixing that constant. Thus scalar factorization cannot hold for arbitrary x∈P,a∈Qx\in P,a\in Q. In a nontracial algebra a scalar trace on all MωM^\omega is not part of the construction in the first place.

The next lesson proves the corrected fast result: equivariance for a countable group of constant lifts, and the identity

Eω(aΦ(x))=Eω(a)Eω(x),x∈P, a∈Q.(19)E_\omega(a\Phi(x))=E_\omega(a)E_\omega(x), \qquad x\in P,\ a\in Q. \tag{19}

For a factor and a centralizing xx, its right side has the scalar factorization suggested by the source. The domain assignment x∈P,a∈Qx\in P,a\in Q is necessary because Φ\Phi is defined on PP.

6. Exercises with complete solutions

Exercise 1. Why does a positive matrix in the quotient have a positive matrix lift for the complete positivity argument?

Solution. The quotient map Mk(Nω)→Mk(Mω)M_k(N_\omega)\to M_k(M^\omega) is surjective. Lift the positive square root of the given matrix to BB, and use B∗BB^*B. Its image is the original positive matrix. Every coordinate of B∗BB^*B is positive, so taking ultraweak limits proves positivity at that matrix level.

Exercise 2. Prove normality of EωE_\omega without interchanging an increasing supremum with an ultralimit.

Solution. Form the supremum YY of the increasing images in the already known von Neumann algebra MM. Positivity gives Y≤Eω(X)Y\le E_\omega(X). The normal state identity (2) gives zero value on their positive difference, as in (4), and faithfulness makes the difference zero. No interchange of two limits is used.

Exercise 3. What changes if MM has a nontrivial center?

Solution. The ultraweak limit of a centralizing representative need only be central, rather than scalar. Equations (10)–(11) still prove a normal Z(M)Z(M)-valued trace. A scalar trace on MωM_\omega is then obtained by composing with a normal state on the original center; different center states can give different scalar traces.

Exercise 4. Check the off-diagonal matrix units in the counterexample.

Solution. Put e=(1+Z)/2e=(1+Z)/2, f=(1−Z)/2f=(1-Z)/2, v=eXfv=eXf. Anticommutation gives Xf=eXXf=eX and Xe=fXXe=fX. Hence vv∗=evv^*=e, v∗v=fv^*v=f, v2=0v^2=0, and e+f=1e+f=1. Together with e,f,v,v∗e,f,v,v^*, these are a unital M2M_2 system. Since Eω(Z)=0E_\omega(Z)=0, both diagonal projections have trace 1/21/2.

Exercise 5. Compute the size of the ambiguity between the two semi-lifts on XX.

Solution. One sends XX to −X-X, and the other sends it to XX. The difference is −2X-2X, with squared trace 22-norm 4τω(X∗X)=44\tau_\omega(X^*X)=4. In particular it is neither zero nor a strong*-null quotient element.

Exercise 6. Explain why covariance with EωE_\omega does not detect this ambiguity.

Solution. The element XX has ultraweak limit zero, so Eω(X)=Eω(−X)=0E_\omega(X)=E_\omega(-X)=0. Both families have identity limit and therefore satisfy (6) with that limit. The faithful expectation detects positive elements faithfully, but it is not an injective linear map on all elements.

Exercise 7. Identify the incompatible requirements in Proposition 5.1.

Solution. Relative commutation with QQ, which contains ZZ, makes the image of XX fixed by Ad⁡(Z)\operatorname{Ad}(Z). Equivariance makes that same image negated because XX is negated in the domain. Over C\mathbb C these equations force zero. This contradiction uses neither a trace-factorization requirement nor failure to fix constants.

Exercise 8. Recover the scalar centralizing version of (19) when MM is a factor.

Solution. If x∈P∩Mωx\in P\cap M_\omega, Theorem 3.1 gives Eω(x)=τω(x)1E_\omega(x)=\tau_\omega(x)1. Equation (19) becomes Eω(aΦ(x))=τω(x)Eω(a)E_\omega(a\Phi(x))=\tau_\omega(x)E_\omega(a). Applying any normal state φ\varphi gives φω(aΦ(x))=τω(x)φω(a)\varphi^\omega(a\Phi(x))=\tau_\omega(x)\varphi^\omega(a). If aa is centralizing too, this is the scalar trace factorization on MωM_\omega. For arbitrary constant xx it need not hold, as (18) shows.

References

Adrian Ocneanu, Actions of discrete amenable groups on factors, thesis, Chapter 5, Section 5.1, printed pp.49–50 (PDF pp.63–64), defines the ultraweak-limit map and states the center-valued trace properties. Section 5.2, printed pp.50–52 (PDF pp.64–66), constructs actions from chosen convergent automorphism families. The direct proofs here supply the positive matrix lifts, faithfulness, normal-state supremum argument and full normal-functional continuity. A given faithful normal state suffices for the expectation and covariance; separable predual is retained for the centralizing algebra.

The Pauli tensor tails give distinct semi-lifts with the same constant restriction and obstruct unrestricted semi-lift equivariance with relative commutation. Constant trace-zero unitaries separately obstruct unqualified scalar factorization. Ocneanu's Fast Reindexation Trick, Section 5.3, printed pp.53–54 (PDF pp.67–68), uses constant lifts and an ordered expectation identity. These hypotheses govern the following lesson. Human-source rights remain separate from the course dedication.