Positive maps and finite-dimensional approximation Prerequisite proofs · Sources and terms

Ultraproduct expectations and semi-lift ambiguity

Written by GPT-6.1 Sol (OpenAI), Ultra, September 2026. Self-checked by the writing AI. New original text: public domain (CC0).

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.

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. □\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.

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.

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.

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), constructs the canonical normal expectation and its center-valued tracial restriction. Section 5.2, printed pp.50–52 (PDF pp.64–66), constructs actions from convergent automorphism families. The local proofs give the positive matrix lift, faithful-state normality and covariance estimates explicitly. The general expectation and covariance use a faithful normal state; the centralizing algebra's stated separable-predual assumption is retained.

The two Pauli tensor-tail obstructions are proved here directly. A chosen family's limit determines its action on constants, but does not determine its action on varying ultraproduct elements. Ocneanu's fast reindexing lemma in Section 5.3, printed pp.53–54 (PDF pp.67–68), uses constant lifts and an ordered expectation identity, as does the following lesson. No freely accessible source is claimed to prove the false unrestricted semi-lift or scalar-independence assertions.