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

Strong stability and tensor absorption

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

An approximately central matrix algebra is a small piece of the hyperfinite factor. Repeatedly placing such pieces in exact relative commutants creates mutually commuting matrix algebras. A summable commutator estimate then forces their infinite product to split off as a spatial tensor factor. This is the mechanism behind strong stability.

We use the central sequence algebra and exact lifting theorem, the noncommutative-corner theorem, and the tracial infinite product and AFD uniqueness proofs. Other inputs are compact-unitary Haar averaging, finite matrix coordinates and normal state GNS representations. The general theory of weights and conditional expectations stays with its designated prerequisite producer; the finite matrix averages used here are constructed explicitly.

1. Stable and strongly stable factors

A factor MM is stable if M≅M⊗ˉMp(C)M\cong M\bar\otimes M_p(\mathbb C) for every positive integer pp. It is strongly stable if

M≅M⊗ˉR,(1)M\cong M\bar\otimes R, \tag{1}

where RR is the separable AFD II1\mathrm{II}_1 factor. These are normal von Neumann algebra isomorphisms.

The product constructions already proved give R⊗ˉR≅RR\bar\otimes R\cong R. For example, the two countable tracial M2M_2 strings can be interleaved into one. Also Mp⊗ˉR≅RM_p\bar\otimes R\cong R: it is a separable AFD II1\mathrm{II}_1 factor, so the finite factor uniqueness theorem applies. Therefore strong stability implies stability.

2. Averaging a finite matrix factor

Let D⊂MD\subset M be a unital copy of Mp(C)M_p(\mathbb C), with matrix units eije_{ij}, and put Dc=D′∩MD^c=D'\cap M. There is a canonical normal matrix decomposition

M≅Mp(Dc),x=∑i,jeijaij,aij=∑kekixejk∈Dc.(2)M\cong M_p(D^c),\qquad x=\sum_{i,j}e_{ij}a_{ij},\qquad a_{ij}=\sum_k e_{ki}xe_{jk}\in D^c. \tag{2}

Indeed, multiplying aija_{ij} on either side by eabe_{ab} gives eaixejbe_{ai}xe_{jb}, so it commutes with every matrix unit. Summing eijaije_{ij}a_{ij} recovers ∑i,jeiixejj=x\sum_{i,j}e_{ii}xe_{jj}=x. Conversely, applying the coefficient formula to eℓmae_{\ell m}a, a∈Dca\in D^c, gives δiℓδjma\delta_{i\ell}\delta_{jm}a. The matrix unit relations show multiplicativity and preservation of adjoints. These finite coordinate maps are normal, and identify the algebra with the spatial product D⊗ˉDcD\bar\otimes D^c.

Define

ED(x)=∫U(D)uxu∗ du=1p∑i,jeijxeji.(3)E_D(x)=\int_{\mathcal U(D)}uxu^*\,du =\frac1p\sum_{i,j}e_{ij}xe_{ji}. \tag{3}

The second expression follows from (2): Haar averaging a scalar matrix keeps its normalized trace, so on D⊗ˉDcD\bar\otimes D^c it is tr⁡p⊗id⁡\operatorname{tr}_p\otimes\operatorname{id}. The finite formula proves normality and complete positivity directly. It is unital, fixes DcD^c, has range DcD^c, and is a DcD^c-bimodule map. It is faithful: if x≥0x\ge0 and ED(x)=0E_D(x)=0, each positive summand eijxejie_{ij}xe_{ji} is zero. In particular eiixeii=0e_{ii}xe_{ii}=0 for every ii, so x1/2eii=0x^{1/2}e_{ii}=0 for every ii, hence x=0x=0.

Lemma 2.1. For every normal functional ψ\psi,

∥ψ−ψ∘ED∥≤p3/2max⁡i,j∥[eij,ψ]∥.(4)\|\psi-\psi\circ E_D\| \le p^{3/2}\max_{i,j}\|[e_{ij},\psi]\|. \tag{4}

If MM has a faithful normal tracial state, then

∥x−ED(x)∥2≤p3/2max⁡i,j∥[eij,x]∥2.(5)\|x-E_D(x)\|_2 \le p^{3/2}\max_{i,j}\|[e_{ij},x]\|_2. \tag{5}

Proof. Averaging first gives

∥ψ−ψ∘ED∥≤∫∥ψ−ψ∘Ad⁡(u)∥ du=∫∥[u,ψ]∥ du.(6)\|\psi-\psi\circ E_D\| \le\int\|\psi-\psi\circ\operatorname{Ad}(u)\|\,du =\int\|[u,\psi]\|\,du. \tag{6}

The predual integrand is norm continuous on the compact finite-dimensional unitary group, so this is a Bochner integral inequality. If u=∑λijeiju=\sum\lambda_{ij}e_{ij}, then ∑∣λij∣2=p\sum|\lambda_{ij}|^2=p. Cauchy–Schwarz gives

∥[u,ψ]∥≤p(∑i,j∥[eij,ψ]∥2)1/2≤p3/2max⁡i,j∥[eij,ψ]∥.(7)\|[u,\psi]\| \le\sqrt p\left(\sum_{i,j}\|[e_{ij},\psi]\|^2\right)^{1/2} \le p^{3/2}\max_{i,j}\|[e_{ij},\psi]\|. \tag{7}

This proves (4). In the tracial case, integrate ∥x−uxu∗∥2=∥[x,u]∥2\|x-uxu^*\|_2=\|[x,u]\|_2 and use the identical coefficient estimate. □\square

3. Summability produces a spatial tensor factor

Theorem 3.1. Let MM have separable predual, without requiring it to be a factor. Let Dν⊂MD_\nu\subset M be mutually commuting unital matrix factors of sizes pνp_\nu, with infinitely many pν≥2p_\nu\ge2. Suppose that for a norm-dense sequence of normal states ψj\psi_j,

∑ν≥1∥ψj−ψj∘EDν∥<∞for every j.(8)\sum_{\nu\ge1}\|\psi_j-\psi_j\circ E_{D_\nu}\|<\infty \qquad\text{for every }j. \tag{8}

Then

R0=⋁ν≥1Dν≅R,M≅R0⊗ˉR0c,R0c=R0′∩M.(9)R_0=\bigvee_{\nu\ge1}D_\nu\cong R,\qquad M\cong R_0\bar\otimes R_0^c, \quad R_0^c=R_0'\cap M. \tag{9}

Proof. Write Eν=EDνE_\nu=E_{D_\nu}. Commuting matrix algebras have commuting conjugation actions, so their averages commute. Each finite composition is a faithful normal conditional expectation onto the intersection of the corresponding commutants.

For N≥mN\ge m, put Fm,N=Em⋯ENF_{m,N}=E_m\cdots E_N. Commutativity and contractivity give, for L>NL>N,

∥ψj∘Fm,L−ψj∘Fm,N∥≤∑ν=N+1L∥ψj−ψj∘Eν∥.(10)\|\psi_j\circ F_{m,L}-\psi_j\circ F_{m,N}\| \le\sum_{\nu=N+1}^L\|\psi_j-\psi_j\circ E_\nu\|. \tag{10}

To see the individual telescoping bound, move the newest EνE_\nu next to ψj\psi_j; the remaining composition is contractive on the predual. The states' linear span is dense in M∗M_*, and all compositions are contractions. Thus ψ∘Fm,N\psi\circ F_{m,N} converges in norm for every ψ∈M∗\psi\in M_*. Its bounded predual limit defines a normal map Tm:M→MT_m:M\to M. Ultraweak limits at every matrix level preserve positivity, so TmT_m is unital completely positive. Its range is

Nm=⋂ν≥mDν′∩M.(11)N_m=\bigcap_{\nu\ge m}D_\nu'\cap M. \tag{11}

Indeed, EνTm=TmE_\nu T_m=T_m for every ν≥m\nu\ge m; conversely all finite compositions fix (11). Their bimodule property passes to the limit, so TmT_m is a conditional expectation onto NmN_m. Also

∥ψj−ψj∘Tm∥≤∑ν≥m∥ψj−ψj∘Eν∥⟶0.(12)\|\psi_j-\psi_j\circ T_m\| \le\sum_{\nu\ge m}\|\psi_j-\psi_j\circ E_\nu\| \longrightarrow0. \tag{12}

Density gives the same convergence for every normal functional; in particular Tm(x)→xT_m(x)\to x ultraweakly.

Let E=T1E=T_1. Its range is R0cR_0^c. Crucially, EE is faithful. For x≥0x\ge0, E(x)=0E(x)=0 implies

(E1⋯Em−1)(Tm(x))=0.(13)(E_1\cdots E_{m-1})(T_m(x))=0. \tag{13}

The finite head composition is faithful, so Tm(x)=0T_m(x)=0. Letting m→∞m\to\infty in (12) gives x=0x=0. Choose a faithful normal state φ\varphi on MM, and set ρ=φ∘E\rho=\varphi\circ E. This is a faithful normal state.

The finite head Am−1=D1∨⋯∨Dm−1A_{m-1}=D_1\vee\cdots\vee D_{m-1} is a full matrix factor: the unital multiplication representation of the tensor product of its commuting full matrix factors is injective, since that finite full matrix algebra is simple. Formula (2) for Am−1A_{m-1} gives

Nm=Am−1∨R0c.(14)N_m=A_{m-1}\vee R_0^c. \tag{14}

In fact, the coefficients of any x∈Nmx\in N_m commute with the head by (2), and with all tail factors because these commute with the head matrix units. They therefore lie in R0cR_0^c. The converse inclusion is immediate. Since Tm(x)∈NmT_m(x)\in N_m and converges ultraweakly to xx, (14) proves

M=R0∨R0c.(15)M=R_0\vee R_0^c. \tag{15}

On a finite head, EE is its normalized trace: the head averages remove it to a scalar and the remaining averages fix that scalar. Thus ρ∣R0\rho|_{R_0} is the normal tracial product state. Its faithfulness and the trace GNS product construction identify R0R_0 normally with the tracial infinite product of the DνD_\nu. Infinitely many nontrivial factors make this a separable AFD II1\mathrm{II}_1 factor, hence R0≅RR_0\cong R. For aa in any finite head and b∈R0cb\in R_0^c, the same average gives

ρ(ab)=τR0(a)φ(b).(16)\rho(ab)=\tau_{R_0}(a)\varphi(b). \tag{16}

Normality extends this to every a∈R0a\in R_0.

Define on the product of the two normal state GNS spaces

aΩτ⊗bΩφ∣R0c⟼abΩρ.(17)a\Omega_{\tau}\otimes b\Omega_{\varphi|_{R_0^c}} \longmapsto ab\Omega_\rho. \tag{17}

Commutation of R0,R0cR_0,R_0^c and (16) show that inner products factor, so (17) is isometric. By (15) and Kaplansky density, products have dense cyclic span in the GNS space of MM, making it onto. It intertwines the two factor actions with their actions in MM. All three GNS representations are faithful and normal because their states are faithful normal. Hence (17) implements the spatial isomorphism (9). □\square

The condition on nontrivial matrix factors is necessary for the type conclusion. If only finitely many pν≥2p_\nu\ge2, the generated R0R_0 is a finite type I matrix factor. Taking every Dν=C1D_\nu=\mathbb C1 satisfies (8) but gives R0=CR_0=\mathbb C. In the absorption application below all sizes are 22.

Theorem 3.2. If MM instead has a faithful normal tracial state τ\tau, the same tensor decomposition follows when

∑ν≥1∥xj−Eν(xj)∥2,τ<∞(18)\sum_{\nu\ge1}\|x_j-E_\nu(x_j)\|_{2,\tau}<\infty \tag{18}

for a 22-norm dense sequence in its unit ball. This conclusion also retains nonfactor algebras.

Proof. All EνE_\nu are trace-preserving 22-norm contractions. Commutativity yields the analogue of (10) on each xjx_j:

∥Fm,L(xj)−Fm,N(xj)∥2≤∑ν=N+1L∥xj−Eν(xj)∥2.(19)\|F_{m,L}(x_j)-F_{m,N}(x_j)\|_2 \le\sum_{\nu=N+1}^L\|x_j-E_\nu(x_j)\|_2. \tag{19}

Density and contraction extend Cauchy convergence to every x∈Mx\in M. The maps' uniform operator norm bounds and completeness of bounded operator balls in the faithful trace 22-topology give limits Tm(x)∈MT_m(x)\in M. These are linear unital completely positive contractions, since bounded 22-convergence gives strong convergence and positivity is strong-closed at every matrix level. They preserve τ\tau.

They are normal. If 0≤xi↑x0\le x_i\uparrow x, let y=sup⁡iTm(xi)≤Tm(x)y=\sup_i T_m(x_i)\le T_m(x). Trace preservation and normality of τ\tau give

τ(Tm(x)−y)=τ(x)−lim⁡iτ(xi)=0,(20)\tau(T_m(x)-y)=\tau(x)-\lim_i\tau(x_i)=0, \tag{20}

so faithfulness gives equality. Their range and bimodule property are (11), by the same commuting-average argument. Moreover Tm(x)→xT_m(x)\to x in 22-norm, by the tails of (18) and density. Thus (14)–(15) hold again.

The head averages show directly τ(ab)=τR0(a)τ(b)\tau(ab)=\tau_{R_0}(a)\tau(b) for a∈R0,b∈R0ca\in R_0,b\in R_0^c, first on finite heads and then by normality. Faithful trace GNS now supplies (17) with ρ=τ\rho=\tau. The same infinite product argument identifies R0≅RR_0\cong R. This proves the entire conclusion without merely substituting a norm in the preceding proof. □\square

4. Removing a fixed finite matrix factor

Lemma 4.1. If MM is a factor with separable predual and D⊂MD\subset M is a unital finite matrix factor, the inclusion Dc⊂MD^c\subset M induces a trace-preserving normal isomorphism

(Dc)ω≅Mω.(21)(D^c)_\omega\cong M_\omega. \tag{21}

Every ordinary centralizing sequence in MM is strong*-equivalent to an ordinary centralizing sequence in DcD^c.

Proof. For a centralizing sequence xnx_n, ordinary or along ω\omega, centrality with each fixed matrix unit and (3) give

ED(xn)−xn=1p∑i,j[eij,xn]eji⟶0strong*.(22)E_D(x_n)-x_n =\frac1p\sum_{i,j}[e_{ij},x_n]e_{ji} \longrightarrow0\quad\text{strong*}. \tag{22}

Fixed right multiplication preserves bounded strong* convergence. The changed sequence remains centralizing in MM by the strong*-small-change estimate.

For sequences already in DcD^c, centralizing in DcD^c and in MM are equivalent. If η∈(Dc)∗\eta\in(D^c)_*, its normal extension η∘ED\eta\circ E_D tests the commutator in MM, using the bimodule property. Conversely, write any z∈Mz\in M in its finite matrix coordinates (2). For ψ∈M∗\psi\in M_*, put ηij(a)=ψ(eija)\eta_{ij}(a)=\psi(e_{ij}a), a∈Dca\in D^c. The coefficients aija_{ij} of a unit-ball zz have norm at most one: each is the amplification of the corner coefficient e1izej1e_{1i}ze_{j1}. Since an x∈Dcx\in D^c commutes with eije_{ij},

∣[x,ψ](z)∣≤∑i,j∥[x,ηij]∥.(23)|[x,\psi](z)| \le\sum_{i,j}\|[x,\eta_{ij}]\|. \tag{23}

This proves the converse at either kind of limit.

Bounded strong* convergence of elements of DcD^c agrees with that in MM, by (2), or by restricting a faithful normal state. Thus inclusion preserves and reflects the zero ideals. It preserves scalar ultraweak limits and the quotient traces. Equation (22) proves surjectivity. A trace-preserving isomorphism of finite von Neumann algebras is normal, by the bounded 22-norm characterization. Finally DcD^c is a factor with separable predual by (2), so its central sequence algebra uses exactly the same hypotheses. □\square

5. Constructing commuting matrix pieces

Theorem 5.1. For a factor MM with separable predual, the following are equivalent:

  1. MM is strongly stable.
  2. MωM_\omega is noncommutative for some free ultrafilter.
  3. MωM_\omega is noncommutative for every free ultrafilter.
  4. MωM_\omega is type II1\mathrm{II}_1 for some, equivalently every, free ultrafilter.
  5. C(M)≠H(M)C(M)\ne H(M).
  6. MM has an ordinary centralizing sequence of mutually commuting unital two-by-two matrix unit systems.

Proof. The preceding hypercentrality and corner theorems equate statements 2–5. We prove the remaining implications constructively.

Suppose M≅N⊗ˉRM\cong N\bar\otimes R, as follows from statement 1 with N=MN=M. The matrix units in successive M2M_2 legs of RR form mutually commuting ordinary centralizing sequences. In the product, 1⊗eij(n)1\otimes e_{ij}(n) remains centralizing: on an elementary normal functional η⊗ζ\eta\otimes\zeta its commutator norm is bounded by ∥η∥∥[eij(n),ζ]∥\|\eta\|\|[e_{ij}(n),\zeta]\|. Finite sums of elementary normal functionals are norm dense in the spatial tensor predual, by approximating its vector functionals with finite tensor sums. Uniform bounds complete the assertion. Transfer by the normal isomorphism gives statement 6.

Conversely, given statement 6, select a subsequence of its matrix systems so that, for a norm-dense normal state sequence ψj\psi_j,

max⁡i,j∥[eij(n),ψk]∥≤2−n,k≤n.(24)\max_{i,j}\|[e_{ij}(n),\psi_k]\|\le2^{-n}, \qquad k\le n. \tag{24}

Mutual commutation survives the subsequence. By Lemma 2.1, the corresponding matrix averages satisfy (8). Theorem 3.1 gives M≅R⊗ˉRcM\cong R\bar\otimes R^c. Therefore

M⊗ˉR≅Rc⊗ˉR⊗ˉR≅Rc⊗ˉR≅M,(25)M\bar\otimes R \cong R^c\bar\otimes R\bar\otimes R \cong R^c\bar\otimes R \cong M, \tag{25}

giving strong stability.

It remains to construct statement 6 from statement 4. Fix ω\omega. The general halving theorem in the finite type II1\mathrm{II}_1 algebra MωM_\omega gives a unital M2M_2 system; its center need not be scalar. We build matrix factors DnD_n inductively, each commuting with the previously generated finite head An−1A_{n-1}, and satisfying (24).

At the first step, lift that quotient M2M_2 system to exact coordinate matrix units in MM. Their ω\omega-centralizing property lets us choose one coordinate satisfying the first finite set of tests. Suppose D1,…,Dn−1D_1,\ldots,D_{n-1} have been chosen. Their commuting unital product An−1A_{n-1} is a finite matrix factor. Lemma 4.1 identifies its relative commutant's central sequence algebra with MωM_\omega, so a unital M2M_2 system exists there. Exact lifting inside An−1′∩MA_{n-1}'\cap M gives matrix units that centralize as sequences in MM, by (23). Choose one coordinate satisfying (24) for k≤nk\le n. It commutes exactly with the entire preceding head.

This induction produces the required mutually commuting systems. The finite tests and their bounds imply ordinary centralizing for every normal functional. This proves statement 6 and completes the equivalence. □\square

For a fixed size p≥2p\ge2, an ordinary centralizing sequence of mutually commuting unital pp-by-pp systems gives the same absorption conclusion: replace 23/22^{3/2} by p3/2p^{3/2} in (4) and use the tracial infinite MpM_p product. The size-one case supplies no absorption information.

6. Exercises with complete solutions

Exercise 1. Verify the coefficient recovery formula in (2) on x=eℓmax=e_{\ell m}a, with a∈Dca\in D^c.

Solution. The coefficient at i,ji,j is ∑kekieℓmaejk=δiℓδmj∑kekka=δiℓδmja\sum_k e_{ki}e_{\ell m}a e_{jk} =\delta_{i\ell}\delta_{mj}\sum_k e_{kk}a =\delta_{i\ell}\delta_{mj}a. Thus each matrix coefficient is recovered exactly. Summing eije_{ij} times those coefficients returns eℓmae_{\ell m}a.

Exercise 2. Derive the constant p3/2p^{3/2} from a unitary's scalar matrix coefficients.

Solution. A unitary pp-by-pp matrix has squared Hilbert–Schmidt norm pp, so (∑∣λij∣2)1/2=p(\sum|\lambda_{ij}|^2)^{1/2}=\sqrt p. There are p2p^2 commutator coefficients, whose square-sum norm is at most pp times their maximum. Multiplying gives p p=p3/2\sqrt p\,p=p^{3/2}.

Exercise 3. In Theorem 3.1, explain why summability for each dense state suffices for every normal functional's Cauchy property.

Solution. Finite linear combinations of the dense states are norm dense in M∗M_*, by positive-functional decomposition. For such a combination, use (10) term by term. Given an arbitrary ψ\psi, approximate it by one such combination η\eta. Since both compositions have predual norm at most one, their difference applied to ψ−η\psi-\eta has norm at most 2∥ψ−η∥2\|\psi-\eta\|. First choose the approximation, then make the Cauchy tail for η\eta small.

Exercise 4. Prove that the infinite average EE is faithful using the tail maps, and explain why faithfulness of the finite averages alone would not justify the conclusion.

Solution. For positive xx with E(x)=0E(x)=0, (13) and faithfulness of the finite head give Tm(x)=0T_m(x)=0 for every mm. Since Tm(x)→xT_m(x)\to x ultraweakly, x=0x=0. A limit of faithful positive maps can lose faithfulness; this argument uses the tail convergence guaranteed by the summability hypothesis, rather than passing faithfulness through a limit without proof.

Exercise 5. Show why infinitely many nontrivial DνD_\nu are needed for R0≅RR_0\cong R.

Solution. If all Dν=C1D_\nu=\mathbb C1, every average is the identity and (8) holds with sum zero, but R0=CR_0=\mathbb C. More generally finitely many nontrivial factors generate a finite full matrix algebra. Infinitely many factors of size at least two give arbitrarily large finite matrix stages and the diffuse tracial infinite product, which is type II1\mathrm{II}_1.

Exercise 6. Verify the isometry of the GNS map (17) on two product vectors.

Solution. Their inner product after mapping is ρ((ab)∗a′b′)=ρ(a∗a′b∗b′)\rho((ab)^*a'b')=\rho(a^*a'b^*b'), because the two algebras commute. Equation (16) makes this τ(a∗a′)φ(b∗b′)\tau(a^*a')\varphi(b^*b'), which is exactly the product Hilbert-space inner product. Bilinearity handles finite sums, so the map extends isometrically.

Exercise 7. In the finite-trace proof, show that trace preservation forces normality of a positive limit map.

Solution. For xi↑xx_i\uparrow x, positivity gives y=sup⁡T(xi)≤T(x)y=\sup T(x_i)\le T(x). Normality of the original faithful trace gives τ(y)=lim⁡τ(T(xi))=lim⁡τ(xi)=τ(x)=τ(T(x))\tau(y)=\lim\tau(T(x_i))=\lim\tau(x_i)=\tau(x)=\tau(T(x)). Thus the positive difference T(x)−yT(x)-y has trace zero and is zero by faithfulness. Preservation of increasing positive suprema is normality.

Exercise 8. Given (24), prove (8) for each fixed ψk\psi_k.

Solution. For n≥kn\ge k, Lemma 2.1 with size two bounds the nn-th defect by 23/22−n2^{3/2}2^{-n}. Their sum is finite. There are only finitely many terms with n<kn<k, each bounded by 2∥ψk∥=22\|\psi_k\|=2, so the entire sum is finite.

Exercise 9. Why can the induction choose DnD_n in the exact relative commutant, even though the original information is asymptotic?

Solution. The finite-head removal isomorphism (21) transfers the exact quotient M2M_2 system into the central sequence algebra of An−1′∩MA_{n-1}'\cap M. The exact matrix lifting theorem then gives coordinate systems already lying in that relative commutant. Selecting one coordinate for the finite functional tests does not change this exact membership. Thus asymptotic centralizing controls the errors, while relative commutant membership ensures exact commutation.

Exercise 10. Give a stable factor which is not strongly stable.

Solution. B(ℓ2(N))⊗ˉMp≅B(ℓ2(N)⊗Cp)≅B(ℓ2(N))B(\ell^2(\mathbb N))\bar\otimes M_p\cong B(\ell^2(\mathbb N)\otimes\mathbb C^p)\cong B(\ell^2(\mathbb N)) for every finite pp, by a Hilbert-space unitary. It is therefore stable. Its central sequence algebra is C\mathbb C, as proved by the rank-one tests in the preceding lifting lesson. Theorem 5.1 excludes strong stability.

References

Alain Connes, Outer conjugacy classes of automorphisms of factors, Lemmas 2.3.5–2.3.6, printed pp.406–407 (PDF pp.25–26), is the free comparison source for finite matrix averaging and summability. Its matrix-functional estimate has constant p². Lemma 2.1 here proves the sharper p^(3/2) bound by averaging the finite matrix coefficients. Theorem 3.1 proves the full normal-functional summability construction for algebras with separable predual, retaining a nontrivial center; infinitely many nontrivial matrix factors are required. Theorem 3.2 supplies the separate finite-trace 2-norm construction.

The proof here establishes faithfulness from the tail maps, proves generation by the tensor factor and its relative commutant, and constructs the spatial isomorphism in the product GNS representation. These steps fill in the finite-factor and modular splitting references used in Connes's proof. The tracial infinite-product construction and finite AFD uniqueness remain separately recorded prerequisites, rather than being declared proved by that citation.

Connes's Theorem 2.2.1 and Lemma 2.2.2, printed pp.400–402 (PDF pp.19–21), compare the central-sequence conditions. Its final absorption implication cites Araki. Here Lemma 4.1 proves finite-head removal in full, and Theorem 5.1 constructs commuting matrix pieces by exact coordinate lifting before applying the summability theorem. The type II₁ central sequence algebra can have nontrivial center; its halving prerequisite retains that scope. The companion automorphism lesson supplies the additional quotient-group and decreasing-subfactor results. No restricted edition is used as construction material and no primary source expression is imported.