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Small corners and the second injective proof

AI-generated exposition by OpenAI GPT models. CC0-1.0 to the extent of rights held.

Finite-dimensional approximation follows from good small corners inside every remaining projection. We prove the local-to-global step by choosing corners with a fixed fraction of the available trace and controlling the finite residual sums. A complete maximality proof gives another route. External finite-rank models and scalar pinching supply the small corners for the separable injective factor conclusion.

We use finite-rank models and repaired internal matrix systems, together with finite trace expectations, TL3. The expectation is normal, completely positive, bimodular and contractive in operator norm, and is the orthogonal projection in the trace Hilbert space. The chain argument uses bounded density on the support corner, BD1–BD5, and the bounded trace topology.

The finite-rank selection and injective-to-small-corner implication concern a separable injective II1\mathrm{II}_1 factor MM, with normalized trace τ\tau. The local-to-global theorem proves a local-to-global implication for every finite algebra with a faithful normal tracial state. The final sequential conclusion retains separable predual. The scalar pinching input uses only the earlier finite expected-subfactor and contained-AFD constructions, so the second proof has its own route to the finite injective conclusion.

The finite-injective factor conclusion

Theorem 4.1. Every injective II1\mathrm{II}_1 factor with separable predual is generated by an increasing sequence of finite-dimensional unital algebras, and is isomorphic to the tracial matrix product RR.

Proof. The small-corner and local-to-global arguments used here are proved below. Proposition 2.2 gives small corners in every nonzero corner. Theorem 3.1 makes MM locally AFD. The earlier exact containment and dyadic construction then supplies an increasing generating dyadic sequence and its trace-GNS identification with RR. □\square

Internal finite-dimensional approximation can be obtained through unitary couplings or through the small-corner condition. Here external finite-rank projections and scalar pinching establish that condition, and either the countable trace-budget argument or maximality gives local AFD. Haagerup's matrix-factorization method and Popa's small-corner method are two approaches to Connes' injectivity and AFD theorem. The general nonfactor finite converse is treated separately in Central disintegration and measurable matrix assembly and Injective algebras and separable tracial envelopes. The factor construction here retains its stated hypotheses.

From small corners to finite approximation

The small-corner condition

Definition 2.1. A faithfully tracial finite algebra has the small-corner approximation property if, for every nonzero projection ee, finite F⊂eMeF\subset eMe, and ε>0\varepsilon>0, there are a nonzero projection f≤ef\le e and a finite-dimensional algebra A⊂fMfA\subset fMf, with identity ff, such that

∥xf−fx∥2≤ετ(f),∥fxf−EA(fxf)∥2≤ετ(f)(x∈F).(12)\|xf-fx\|_2\le\varepsilon\sqrt{\tau(f)},\qquad \|fxf-E_A(fxf)\|_2\le\varepsilon\sqrt{\tau(f)} \quad(x\in F). \tag{12}

This is the local finite-dimensional condition used in the references below. It is stronger than merely finding good matrix coefficients in some corner: the corner must also almost commute with the tests, and the condition is required inside every nonzero corner.

Finite approximation by trace budgets and maximality

Theorem 3.1. A finite von Neumann algebra with faithful normal tracial state and the small-corner property is locally AFD. This implication requires neither factoriality nor separable predual.

Proof by a countable trace budget. Fix a finite list FF of contractions in MM and a target error ε>0\varepsilon>0. The empty list is approximated by C1\mathbb C1, so suppose F≠∅F\ne\varnothing. Put

c=ε/2.(SCG1)c=\varepsilon/2. \tag{SCG1}

For a nonzero projection ee, call a pair (g,B)(g,B) admissible in ee if 0≠g≤e0\ne g\le e, B⊂gMgB\subset gMg is a finite-dimensional algebra with identity gg, and

∥[exe,g]∥2≤cτ(g),∥gxg−EB(gxg)∥2≤cτ(g)(x∈F).(SCG2)\|[exe,g]\|_2\le c\sqrt{\tau(g)}, \qquad \|gxg-E_B(gxg)\|_2\le c\sqrt{\tau(g)} \quad(x\in F). \tag{SCG2}

The small-corner property, applied to eFeeFe, supplies such a pair. Consequently the real number

σ(e)=sup⁡{τ(g):(g,B) is admissible in e}\sigma(e)=\sup\{\tau(g):(g,B)\text{ is admissible in }e\}

is defined and satisfies 0<σ(e)≤τ(e)0<\sigma(e)\le\tau(e).

Start with e0=1e_0=1. If en≠0e_n\ne0, choose an admissible pair (gn,Bn)(g_n,B_n) in ene_n such that

τ(gn)>12σ(en),en+1=en−gn.(SCG3)\tau(g_n)>\tfrac12\sigma(e_n), \qquad e_{n+1}=e_n-g_n. \tag{SCG3}

The choice exists by the defining property of the supremum. Stop if a remaining projection is zero. The gng_n's are mutually orthogonal, and

∑nτ(gn)≤1.\sum_n\tau(g_n)\le1.

If the construction is infinite, it follows that τ(gn)→0\tau(g_n)\to0 and hence σ(en)→0\sigma(e_n)\to0.

We prove that the remaining trace tends to zero. For an infinite construction, let e∞=⋀nene_\infty=\bigwedge_n e_n. Decreasing projections converge strongly to the projection onto the intersection of their ranges: for m≥nm\ge n,

∥(en−em)ξ∥2=∥enξ∥2−∥emξ∥2,\|(e_n-e_m)\xi\|^2 =\|e_n\xi\|^2-\|e_m\xi\|^2,

so the vector sequence is Cauchy and its limit is that intersection projection. Strong closure puts e∞e_\infty in MM. Normality of the finite trace gives

∥en−e∞∥22=τ(en)−τ(e∞)⟶0.(SCG4)\|e_n-e_\infty\|_2^2 =\tau(e_n)-\tau(e_\infty)\longrightarrow0. \tag{SCG4}

Suppose e∞≠0e_\infty\ne0. Apply the small-corner property in this remaining corner with the smaller tolerance c/2c/2. Obtain 0≠g≤e∞0\ne g\le e_\infty and a finite-dimensional B⊂gMgB\subset gMg with identity gg, such that both errors for the compressed tests e∞xe∞e_\infty x e_\infty are at most (c/2)τ(g)(c/2)\sqrt{\tau(g)}.

This fixed pair is admissible in ene_n for all sufficiently large nn. Indeed g≤e∞≤eng\le e_\infty\le e_n, so

g(enxen)g=gxg=g(e∞xe∞)g.g(e_nxe_n)g=gxg=g(e_\infty x e_\infty)g.

Thus its diagonal approximation error does not change. For the commutator,

[enxen,g]−[e∞xe∞,g]=(en−e∞)xg−gx(en−e∞),∥[enxen,g]−[e∞xe∞,g]∥2≤2∥x∥∥en−e∞∥2⟶0.(SCG5)\begin{aligned} [e_nxe_n,g]-[e_\infty x e_\infty,g] &=(e_n-e_\infty)xg-gx(e_n-e_\infty),\\ \|[e_nxe_n,g]-[e_\infty x e_\infty,g]\|_2 &\le2\|x\|\|e_n-e_\infty\|_2\longrightarrow0. \end{aligned} \tag{SCG5}

The finite list permits one common sufficiently large index, for which this last norm is less than (c/2)τ(g)(c/2)\sqrt{\tau(g)}. Hence (SCG2) holds for (g,B)(g,B) in every later ene_n. It follows that σ(en)≥τ(g)>0\sigma(e_n)\ge\tau(g)>0, contradicting σ(en)→0\sigma(e_n)\to0. Therefore e∞=0e_\infty=0 and τ(en)→0\tau(e_n)\to0. This argument does not require the numbers σ(en)\sigma(e_n) themselves to be monotone.

We now keep the complete quantitative approximation error. Set

bn(x)=EBn(gnxgn),RN(x)=x−eNxeN−∑n<Nbn(x).b_n(x)=E_{B_n}(g_nxg_n), \qquad R_N(x)=x-e_Nxe_N-\sum_{n<N}b_n(x).

Then R0(x)=0R_0(x)=0, and

Rn+1(x)=Rn(x)+Sn(x),Sn(x)=enxen−en+1xen+1−bn(x).R_{n+1}(x)=R_n(x)+S_n(x), \qquad S_n(x)=e_nxe_n-e_{n+1}xe_{n+1}-b_n(x).

The compression of Rn(x)R_n(x) to enMene_nMe_n is zero, while Sn(x)S_n(x) belongs to that corner. Cyclicity therefore makes the two terms orthogonal in L2L^2. With y=enxeny=e_nxe_n, the three ordered corner blocks of Sn(x)S_n(x) are

en+1ygn,gnyen+1,gnygn−EBn(gnygn).e_{n+1}yg_n,\qquad g_nye_{n+1},\qquad g_nyg_n-E_{B_n}(g_nyg_n).

They are mutually orthogonal. The first two squared norms sum to ∥[y,gn]∥22\|[y,g_n]\|_2^2, since the two blocks of this commutator differ only in the sign of one block. Admissibility now gives

∥Sn(x)∥22≤2c2τ(gn),∥RN(x)∥22≤2c2∑n<Nτ(gn)≤ε2/2.(SCG6)\|S_n(x)\|_2^2\le2c^2\tau(g_n), \qquad \|R_N(x)\|_2^2 \le2c^2\sum_{n<N}\tau(g_n)\le\varepsilon^2/2. \tag{SCG6}

Only finite sums have been used in this estimate.

For every available finite NN, form the finite-dimensional unital subalgebra

DN=(⨁n<NBn)⊕CeN.(SCG7)D_N=\left(\bigoplus_{n<N}B_n\right)\oplus\mathbb C e_N. \tag{SCG7}

The orthogonal supports sum to 1−eN1-e_N, so the displayed algebra has identity 11; omit the zero scalar summand if eN=0e_N=0. The element ∑n<Nbn(x)\sum_{n<N}b_n(x) belongs to DND_N. Thus

dist⁡2(x,DN)≤∥x−∑n<Nbn(x)∥2≤∥RN(x)∥2+∥eNxeN∥2≤ε/2+τ(eN).(SCG8)\begin{aligned} \operatorname{dist}_2(x,D_N) &\le\left\|x-\sum_{n<N}b_n(x)\right\|_2\\ &\le\|R_N(x)\|_2+\|e_Nxe_N\|_2\\ &\le\varepsilon/\sqrt2+\sqrt{\tau(e_N)} . \end{aligned} \tag{SCG8}

If the construction terminates, use its terminal NN. Otherwise choose NN so large that τ(eN)<ε(1−1/2)\sqrt{\tau(e_N)}<\varepsilon(1-1/\sqrt2). In either case every x∈Fx\in F has distance less than ε\varepsilon from this one finite-dimensional unital algebra. Its trace expectation is the L2L^2 nearest-point map, so EDN(x)E_{D_N}(x) gives the same error bound and satisfies ∥EDN(x)∥≤∥x∥\|E_{D_N}(x)\|\le\|x\|.

Arbitrary finite bounded lists reduce to contractions by a common scalar rescaling. We have proved local AFD for every finite von Neumann algebra with the stated faithful normal tracial state. The countable construction is chosen for each finite test list; no countable dense subset, factoriality or separable-predual assumption is used. □\square

Second proof, by maximality. Fix a finite contraction list F⊂MF\subset M and ε>0\varepsilon>0. Consider all locally AFD von Neumann subalgebras A⊂MA\subset M, permitting identity f≠1f\ne1 and the zero algebra, which satisfy

∥x−(1−f)x(1−f)−EA(fxf)∥2≤ετ(f)(x∈F).(13)\|x-(1-f)x(1-f)-E_A(fxf)\|_2 \le\varepsilon\sqrt{\tau(f)} \qquad(x\in F). \tag{13}

Here EA(fxf)E_A(fxf) is the normal trace expectation in fMffMf, extended to MM by compression. Order these algebras by inclusion.

We verify the chain condition. For an increasing chain AiA_i, let fif_i be its supports and f=sup⁡ifif=\sup_i f_i. Take AA to be the nonunital strong operator closure of ⋃iAi\bigcup_i A_i in MM. If f=0f=0, this is the zero algebra and already an upper bound. If f≠0f\ne0, the union acts nondegenerately on fHfH, since fi→ff_i\to f strongly. Its bicommutant on fHfH, extended by zero on (1−f)H(1-f)H, is precisely AA, with identity ff. In particular we do not take the ambient bicommutant on all of HH, which would adjoin the complementary scalar identity.

This AA is locally AFD: Kaplansky approximation for the nondegenerate algebra on fHfH gives bounded L2L^2 approximants from the union to any finite list in AA; approximate that finite list further inside one chain member. Add the scalar algebra C(f−fi)\mathbb C(f-f_i) to make the resulting finite algebra unital in AA.

The closed spaces L2(Ai)L^2(A_i) increase to L2(A)L^2(A), so their orthogonal projections converge strongly. These projections are precisely x↦EAi(fixfi)x\mapsto E_{A_i}(f_i x f_i). Also (1−fi)x(1−fi)→(1−f)x(1−f)(1-f_i)x(1-f_i)\to(1-f)x(1-f) in L2L^2, by bounded strong convergence and the finite trace. Therefore (13) passes to AA. Every chain has an upper bound in the set, and Zorn's lemma supplies a maximal AA.

To justify the projection limit directly, split a Hilbert vector into its projection onto the closed union and its orthogonal remainder. Every projection in the chain annihilates the remainder. Approximate the first part by a vector in one chain subspace; every later orthogonal projection fixes that approximant, and contractivity bounds the remaining error by its distance from the first part. This proves strong convergence for the whole directed chain. Bounded density on the support corner, applied to the trace vector, proves the required density of the union in the trace Hilbert space. Thus the argument uses nets and does not assume a countable chain.

Suppose f≠1f\ne1, and put e=1−fe=1-f. Apply (12) in eMeeMe to eFeeFe, with tolerance ε/2\varepsilon/2. Obtain g≠0g\ne0, g≤eg\le e, and a finite-dimensional B⊂gMgB\subset gMg. For y=exey=exe, set

R=x−exe−EA(fxf),S=y−(e−g)y(e−g)−EB(gyg).(14)R=x-e x e-E_A(fxf),\qquad S=y-(e-g)y(e-g)-E_B(gyg). \tag{14}

Every block of RR has at least one ff coordinate, whereas S∈eMeS\in eMe; they are orthogonal in L2L^2. The three blocks of SS are

(e−g)yg,gy(e−g),gyg−EB(gyg).(e-g)yg,\quad gy(e-g),\quad gyg-E_B(gyg).

They are mutually orthogonal. The first two squared norms sum to ∥yg−gy∥22\|yg-gy\|_2^2. Condition (12) therefore gives

∥S∥22≤ε22τ(g).(15)\|S\|_2^2\le\frac{\varepsilon^2}{2}\tau(g). \tag{15}

For L=A⊕BL=A\oplus B, identity h=f+gh=f+g, its residual in (13) is R+SR+S, so

∥R+S∥22≤ε2τ(f)+ε22τ(g)≤ε2τ(h).(16)\|R+S\|_2^2\le\varepsilon^2\tau(f) +\frac{\varepsilon^2}{2}\tau(g) \le\varepsilon^2\tau(h). \tag{16}

The direct sum is locally AFD and strictly contains AA, contradicting maximality. Thus f=1f=1, and (13) gives ∥x−EA(x)∥2≤ε\|x-E_A(x)\|_2\le\varepsilon for all x∈Fx\in F.

Approximate the finitely many EA(x)E_A(x)'s by a finite-dimensional unital algebra of AA. Choosing both this new error and the original ε\varepsilon arbitrarily small proves local AFD of MM. The expectation onto the final finite algebra supplies approximants of norm at most one. □\square

For a separable II1\mathrm{II}_1 factor, local AFD also implies the small-corner property. The finite amplification and corner permanence proof is valid without separability. Inside a nonzero corner approximate the finite tests by a unital finite-dimensional algebra and take f=ef=e; its commutator error is zero. Thus the source's LAFD and AFD conditions are equivalent at their stated hypotheses.

Obtaining small corners in injective factors

Proposition 2.2. Every injective II1\mathrm{II}_1 factor with separable predual has this property.

Proof. The almost invariant matrix-corner selection used here is proved in the next section. For finite unitary tests in MM, Lemma 1.1, (11) and the two-parameter choice give (12), since ∥vs−sv∥2=∥vsv∗−s∥2\|v s-sv\|_2=\|v s v^*-s\|_2.

Every bounded element is a scalar linear combination of at most four unitaries. For a self-adjoint contraction hh, write h=(u+u∗)/2h=(u+u^*)/2 with u=h+i(1−h2)1/2u=h+i(1-h^2)^{1/2}; apply this to the real and imaginary parts and rescale. For a finite operator list, take the union of these unitary lists. Divide the unitary tolerance by the largest sum of absolute coefficients, using 11 if that sum is zero. Linearity, the triangle inequality and linearity of EAE_A give (12) for the operator list.

Finally every nonzero eMeeMe is an injective II1\mathrm{II}_1 factor with separable predual, by corner compression of a retraction and finite factor comparison. Repeat the argument with its normalized trace τe=τ/τ(e)\tau_e=\tau/\tau(e). Both sides of (12) acquire the same factor τ(e)\sqrt{\tau(e)} when converted to the ambient trace. □\square

Here the corner assertions have separate elementary reasons. The center-of-a-corner proof makes a nonzero corner of a factor a factor. It has no minimal projection: a minimal projection in the corner would also be minimal in the original algebra. Its restricted trace is faithful, normal and finite. Every normal functional on the corner extends normally to the ambient algebra by compression, so restriction makes its predual a quotient of the separable ambient predual. Injectivity itself is the completely positive extension and compression argument of Lemma 6.1; it does not require a normal retraction.

Selecting an almost invariant matrix model

Fix a finite F⊂U(M)F\subset\mathcal U(M) containing 11, and first choose a finite-rank model

q=∑i=1mKxi,xi,∑v∈F∥vqv∗−q∥HS2<a2m,(1)q=\sum_{i=1}^m K_{x_i,x_i},\qquad \sum_{v\in F}\|v q v^*-q\|_{\mathrm{HS}}^2<a^2m, \tag{1}

with xi∈Mx_i\in M orthonormal in L2L^2. The number a>0a>0 is the first approximation parameter. This choice fixes mm and B≥max⁡(1,∥xi∥)B\ge\max(1,\|x_i\|). Only after that choice do we make the Gram and pinching parameter bb small.

Use the preceding lesson's Corollary 3.1, and abbreviate its moduli by D=Dm(b)D=D_m(b), d=dm(b)d=d_m(b). It gives orthogonal initial projections eke_k, repaired vectors wi(k)w_i(k), matrix units Eij(k)E_{ij}(k) and their supports sks_k. Write p=∑kekp=\sum_k e_k. By making bb small with m,Bm,B fixed, arrange

τ(1−p)<12B2.(2)\tau(1-p)<\frac1{2B^2}. \tag{2}

Then each ∥xip∥22≥1−B2τ(1−p)>1/2\|x_i p\|_2^2\ge1-B^2\tau(1-p)>1/2.

Lemma 1.1. For some kk, putting s=sks=s_k and

Cv=∑i,jτ(xi∗vxj)Eij(k),C_v=\sum_{i,j}\tau(x_i^*v x_j)E_{ij}(k),

we have, for every v∈Fv\in F,

∥svs−Cv∥2≤m dτ(s),∥vsv∗−s∥2≤η2+2m dτ(s),η=2D+2 a(1+D).(3)\begin{aligned} \|s v s-C_v\|_2&\le\sqrt m\,d\sqrt{\tau(s)},\\ \|v s v^*-s\|_2&\le \sqrt{\eta^2+2\sqrt m\,d}\sqrt{\tau(s)},\\ \eta&=2D+\sqrt2\,a(1+D). \end{aligned} \tag{3}

Proof. Let Qk=∑iKxiek,xi=RekqQ_k=\sum_i K_{x_i e_k,x_i}=R_{e_k}q, where RekR_{e_k} means right multiplication on the output vector. The operator RekR_{e_k} is an orthogonal projection on HH, commuting with every LvL_v. For each vv, the operators Rek(vqv∗−q)R_{e_k}(v q v^*-q) are orthogonal in Hilbert–Schmidt space. Thus

∑k,v∥vQkv∗−Qk∥HS2<a2m.(4)\sum_{k,v}\|v Q_kv^*-Q_k\|_{\mathrm{HS}}^2<a^2m. \tag{4}

Orthonormality of the second vectors in QkQ_k gives

∑k∥Qk∥HS2=∑i∥xip∥22>m/2.(5)\sum_k\|Q_k\|_{\mathrm{HS}}^2 =\sum_i\|x_i p\|_2^2>m/2. \tag{5}

Consequently there is kk with summed error less than 2a2∥Qk∥HS22a^2\|Q_k\|_{\mathrm{HS}}^2. This QkQ_k is nonzero.

Put V=∑iKwi(k),xiV=\sum_i K_{w_i(k),x_i}. The same orthonormality and the repaired vector errors give

∥V−Qk∥HS≤D∥V∥HS,∥V∥HS2=mτ(ek)=τ(s).(6)\|V-Q_k\|_{\mathrm{HS}}\le D\|V\|_{\mathrm{HS}},\qquad \|V\|_{\mathrm{HS}}^2=m\tau(e_k)=\tau(s). \tag{6}

The triangle inequality, applied to each test and to its conjugate, therefore gives

∥vVv∗−V∥HS≤ητ(s).(7)\|v Vv^*-V\|_{\mathrm{HS}}\le\eta\sqrt{\tau(s)}. \tag{7}

The first inequality in (3) is the matrix coefficient estimate already proved. To obtain the second, expand the rank-one Hilbert–Schmidt pairing:

∥vVv∗−V∥HS2=2τ(s)−2Re⁡τ(Cv∗v).(8)\|v Vv^*-V\|_{\mathrm{HS}}^2 =2\tau(s)-2\operatorname{Re}\tau(C_v^*v). \tag{8}

Indeed its cross term is ∑i,jτ(wi∗vwj)τ(xi∗vxj)‾\sum_{i,j}\tau(w_i^*v w_j)\overline{\tau(x_i^*v x_j)}, equal to τ(Cv∗v)\tau(C_v^*v). Both CvC_v and svss v s are supported by ss. Hence

∣τ((Cv−svs)∗v)∣≤∥Cv−svs∥2∥svs∥2≤m d τ(s).(9)\begin{aligned} |\tau((C_v-s v s)^*v)| &\le\|C_v-s v s\|_2\|s v s\|_2\\ &\le\sqrt m\,d\,\tau(s). \end{aligned} \tag{9}

Also

2τ(s)−2τ(sv∗sv)=∥vsv∗−s∥22.(10)2\tau(s)-2\tau(s v^*s v)=\|v s v^*-s\|_2^2. \tag{10}

Combining (7)–(10) proves the second bound in (3). □\square

Let Ak=span⁡{Eij(k)}A_k=\operatorname{span}\{E_{ij}(k)\}, a matrix algebra with identity ss. The L2L^2 nearest-point property of its trace expectation gives

∥svs−EAk(svs)∥2≤m dτ(s).(11)\|s v s-E_{A_k}(s v s)\|_2\le\sqrt m\,d\sqrt{\tau(s)}. \tag{11}

Given any desired small tolerance c>0c>0, first choose aa so 2 a<c/2\sqrt2\,a<c/2. Then fix the model (1), and decrease bb until (2) holds and both m d<c\sqrt m\,d<c and η2+2m d<c\sqrt{\eta^2+2\sqrt m\,d}<c. This is possible because m,Bm,B are now fixed and D,d→0D,d\to0. Allowing the dimension of the first model to vary while taking the second limit would not justify these inequalities.

5. Exercises with complete solutions

Global approximation and residual budgets

Exercise 7. Why is chain closure of the algebras alone insufficient for the Zorn argument?

Solution. An upper bound must also satisfy the quantitative residual condition (13). The increasing L2L^2 subspaces give strong convergence of their expectation projections, while the increasing supports give convergence of the complementary compressions. These two limits and normality of the trace pass the inequality to the generated algebra.

Exercise 8. Verify the squared error budget (15).

Solution. The two off-diagonal blocks have squared sum ∥yg−gy∥22≤(ε2/4)τ(g)\|yg-gy\|_2^2\le(\varepsilon^2/4)\tau(g). The diagonal approximation error has the same squared bound. Orthogonality gives their sum at most (ε2/2)τ(g)(\varepsilon^2/2)\tau(g). Its normalization uses the new support gg.

Exercise 9. Why does the maximal algebra supply bounded finite-dimensional approximants to the original xx's?

Solution. At full support its expectation approximates the xx's within the first tolerance. Its local AFD property supplies a finite algebra DD approximating those finitely many expectations. The triangle inequality bounds the distance of each xx to DD. The tracial nearest-point property bounds ∥x−ED(x)∥2\|x-E_D(x)\|_2 by that distance, and contractivity gives ∥ED(x)∥≤∥x∥\|E_D(x)\|\le\|x\|.

Exercise 10. Which nonfactor statement is proved here, and what remains open?

Solution. The small-corner-to-local-AFD implication of Theorem 3.1 holds in every finite algebra with faithful normal trace. The proof that an injective algebra has small corners uses scalar pinching in a separable II1\mathrm{II}_1 factor. Thus this route proves the full second factor argument, while the general nonfactor injective converse and its central decomposition consequences still need their separate proof.

Finite-rank selection and corner scales

Exercise 1. Why is the right multiplication projection RekR_{e_k} orthogonal on L2(M,τ)L^2(M,\tau)?

Solution. It is idempotent because ek2=eke_k^2=e_k. Its adjoint is itself: τ((ξek)∗ζ)=τ(ekξ∗ζ)=τ(ξ∗ζek)\tau((\xi e_k)^*\zeta)=\tau(e_k\xi^*\zeta)=\tau(\xi^*\zeta e_k). For orthogonal ek,ele_k,e_l, the corresponding projections have zero product. Left multiplication commutes with them, since v(ξek)=(vξ)ekv(\xi e_k)=(v\xi)e_k.

Exercise 2. Prove the lower bound in (5).

Solution. Orthonormality of the second rank-one vectors xix_i removes all cross terms, giving ∥Qk∥HS2=∑i∥xiek∥22\|Q_k\|_{\mathrm{HS}}^2=\sum_i\|x_i e_k\|_2^2. Summing over the orthogonal eke_k's gives ∑i∥xip∥22\sum_i\|x_i p\|_2^2. Each is 1−τ(xi∗xi(1−p))≥1−B2τ(1−p)>1/21-\tau(x_i^*x_i(1-p))\ge1-B^2\tau(1-p)>1/2.

Exercise 3. Justify selection of kk between (4) and (5).

Solution. If every nonzero QkQ_k had summed error at least 2a2∥Qk∥HS22a^2\|Q_k\|_{\mathrm{HS}}^2, the total error would exceed a2ma^2m by (5), contradicting (4). A zero QkQ_k has zero conjugation error and contributes nothing, so it does not affect this argument.

Exercise 4. Check the conjugates in the cross term (8).

Solution. The rank-one pairing gives τ(wi∗vwj)τ((vxj)∗xi)=τ(wi∗vwj)τ(xi∗vxj)‾\tau(w_i^*v w_j)\tau((v x_j)^*x_i)=\tau(w_i^*v w_j)\overline{\tau(x_i^*v x_j)}. Since Eji=wjwi∗E_{ji}=w_jw_i^*, cyclicity gives τ(Ejiv)=τ(wi∗vwj)\tau(E_{ji}v)=\tau(w_i^*v w_j). Summing yields τ(Cv∗v)\tau(C_v^*v).

Exercise 5. Explain the two independent parameters in the proof.

Solution. The finite-rank model chosen at tolerance aa determines mm and BB. The Gram repair moduli tend to zero with bb only for those fixed values. First choose aa to make 2a\sqrt2a small, then fix the model, then make bb small enough to control Dm(b)D_m(b), m dm(b)\sqrt m\,d_m(b) and the uncovered trace. This proves every bound in (3) simultaneously.

Exercise 6. Convert (12) from a normalized corner trace to the ambient trace.

Solution. In eMeeMe, ∥z∥2,e=∥z∥2/τ(e)\|z\|_{2,e}=\|z\|_2/\sqrt{\tau(e)}, while τe(f)=τ(f)/τ(e)\tau_e(f)=\tau(f)/\tau(e). Multiply an inequality ∥z∥2,e≤ετe(f)\|z\|_{2,e}\le\varepsilon\sqrt{\tau_e(f)} by τ(e)\sqrt{\tau(e)}. Both factors cancel, leaving (12).

References and proof scope

Sorin Popa, A short proof of “injectivity implies hyperfiniteness” for finite von Neumann algebras, Journal of Operator Theory 16 (1986), 261–272, Proposition 2.2 and Section 3. The small-corner and maximality methods are credited to this work. Popa constructs finite approximation in general finite algebras through an abelian-module argument. The external Hilbert-space finite-rank selection used here instead retains the separable factor hypothesis of its scalar-pinching input.

Claire Anantharaman and Sorin Popa, An introduction to II₁ factors, author draft, Definition 11.1.4 and Theorem 11.1.5, pp.174 and 182–184, develop the abelian-module small-corner method. Theorem 11.1.17, pp.184–185, uses maximal orthogonal families to pass from local corners to finite approximation. The complete maximality proof here supplies support-corner closure, bounded density, the expectation-projection limit and the precise orthogonal residual budget.

The countable proof chooses each new corner with more than half the supremum of the traces available at the fixed tolerance. A hypothetical nonzero remaining corner gives a fixed smaller-tolerance candidate which eventually works at every finite stage. This forces the remaining trace to vanish. Finite orthogonal residual sums then give an actual finite-dimensional unital approximating algebra. This proof requires neither factoriality nor separable predual.

The final increasing dyadic sequence and the identification with RR use the complete exact-containment and dyadic construction. They are separate from the arbitrary finite local-to-global implication. The general nonfactor injective converse has its own central-disintegration and tracial-envelope proofs.