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

Operator density from finite vector tests

Written by GPT-6.1 Sol (OpenAI), Ultra, October 2026. Original text and embedded diagram: public domain (CC0).

A strong operator neighbourhood asks for good approximation on finitely many vectors. Commutants turn those finite tests into one invariant-subspace problem. A rational function then converts self-adjoint approximants into contractions. These two constructions prove the positive matrix density needed to reconstruct completely positive maps with values in a C*-algebra.

We use the complete Hilbert-space, projection and series-vector proofs H00–H03, their arbitrary-Hilbert-space identification P00, C*-unitization, calculus and approximate identities F02–F09, and real convex separation SEP. The C*-norm and order on finite matrices, including entrywise representations, are proved in Completely positive maps, Section 2. Inner products are linear in their second variable. No separability assumption is imposed.

For a representation π:A→B(H)\pi:A\to B(H), put

D=π(A),K=DH‾,P=PK.D=\pi(A),\qquad K=\overline{D H},\qquad P=P_K.

The notation DH‾\overline{D H} means the closed linear span. We work on KK, and extend operators on KK by zero on K⊥K^\perp whenever the original space HH is used. Write

M=(D∣K)′′,M=(D|_K)'',

where these commutants are taken in B(K)B(K). The unit of this algebra on HH is PP. When K=0K=0, all supported operators and all the approximations below are zero.

ODF01. Bounded strong limits and ultraweak tests

Strong convergence means Tiξ→TξT_i\xi\to T\xi in norm for every vector ξ\xi. Weak operator convergence means convergence of every scalar ⟨η,Tiξ⟩\langle\eta,T_i\xi\rangle. Strong* convergence means that both Ti→TT_i\to T and Ti∗→T∗T_i^*\to T^* strongly. H03 describes the ultraweak topology by the functionals

T⟼∑j=1∞⟨ηj,Tξj⟩,∑j∥ηj∥∥ξj∥<∞.(ODF1)T\longmapsto\sum_{j=1}^{\infty}\langle\eta_j,T\xi_j\rangle, \qquad \sum_j\|\eta_j\|\|\xi_j\|<\infty. \tag{ODF1}

P00 makes that description available on every Hilbert space, including spaces with uncountable orthonormal bases.

Bounded product lemma. If Si→SS_i\to S and Ti→TT_i\to T strongly and sup⁡i∥Si∥≤C<∞\sup_i\|S_i\|\le C<\infty, then SiTi→STS_iT_i\to ST strongly.

Proof. For each ξ\xi,

∥(SiTi−ST)ξ∥≤C∥(Ti−T)ξ∥+∥(Si−S)Tξ∥⟶0.\|(S_iT_i-ST)\xi\| \le C\|(T_i-T)\xi\|+\|(S_i-S)T\xi\|\longrightarrow0.

The last vector TξT\xi is fixed. No bound on the norms of the TiT_i is needed for this assertion. If both nets and their adjoints converge strongly and both nets have uniform norm bounds, applying the same argument to Ti∗Si∗T_i^*S_i^* also proves strong* convergence of the products. □\square

Bounded topology lemma. If Ti→TT_i\to T in the weak operator topology and sup⁡i∥Ti∥≤C\sup_i\|T_i\|\le C, then Ti→TT_i\to T ultraweakly. In particular every uniformly bounded strongly convergent net converges ultraweakly.

Proof. For unit vectors η,ξ\eta,\xi, the scalar limit gives ∣⟨η,Tξ⟩∣≤C|\langle\eta,T\xi\rangle|\le C, and the Hilbert norming formula gives ∥T∥≤C\|T\|\le C. Given (ODF1), its tail after NN, evaluated at Ti−TT_i-T, has modulus at most

2C∑j>N∥ηj∥∥ξj∥.2C\sum_{j>N}\|\eta_j\|\|\xi_j\|.

Choose NN to make this small. The initial finite sum tends to zero by weak operator convergence, so the whole series tends to zero. If C=0C=0, every operator involved is zero. This is a net argument: convergence of the finite sum requires only finitely many eventual conditions. □\square

The uniform bounds in these lemmas are hypotheses. Strong convergence of an arbitrary net supplies no uniform operator-norm bound by itself.

ODF02. The essential representation and its support

Every d∈Dd\in D preserves KK. Since D=D∗D=D^*, it also preserves K⊥K^\perp. A vector ζ∈K⊥\zeta\in K^\perp satisfies ⟨d∗η,ζ⟩=0\langle d^*\eta,\zeta\rangle=0 for every d∈Dd\in D, η∈H\eta\in H, so dζ=0d\zeta=0. Thus d=PdPd=PdP.

Let (eλ)(e_\lambda) be the positive contractive approximate identity in AA supplied by F09. On a vector π(a)η\pi(a)\eta,

π(eλ)π(a)η=π(eλa)η⟶π(a)η.\pi(e_\lambda)\pi(a)\eta=\pi(e_\lambda a)\eta \longrightarrow\pi(a)\eta.

F05 gives ∥π(eλ)∥≤1\|\pi(e_\lambda)\|\le1. Finite sums of these vectors are dense in KK; the uniform bound extends convergence to all of KK. Every π(eλ)\pi(e_\lambda) vanishes on K⊥K^\perp. Consequently

π(eλ)⟶Pstrongly on H.(ODF2)\pi(e_\lambda)\longrightarrow P\quad\hbox{strongly on }H. \tag{ODF2}

On KK, this is a strongly convergent approximate identity with limit 1K1_K. In particular the restricted representation is nondegenerate. These statements include A=0A=0 and π=0\pi=0.

The supported algebra MM, rather than the full bicommutant in a degenerate ambient space, is the closure to be approximated. For example, if D=0D=0 on a nonzero HH, its strong closure is zero although its full bicommutant contains 1H1_H.

ODF03. The bicommutant theorem on finitely many vectors

Theorem. On KK, DD is strongly dense in M=D′′M=D''. More precisely, for T∈MT\in M, ξ1,…,ξr∈K\xi_1,\ldots,\xi_r\in K, and ε>0\varepsilon>0, there is a∈Aa\in A such that

∑j=1r∥(π(a)−T)ξj∥2<ε2.(ODF3)\sum_{j=1}^r\|(\pi(a)-T)\xi_j\|^2<\varepsilon^2. \tag{ODF3}

Proof. The zero essential space and the assertion with no test vectors are immediate: take a=0a=0. For r≥1r\ge1, write ξ=(ξ1,…,ξr)∈Kr\boldsymbol\xi=(\xi_1,\ldots,\xi_r)\in K^r, and consider the closed linear subspace

L={(dξ1,…,dξr):d∈D}‾⊂Kr.L=\overline{\{(d\xi_1,\ldots,d\xi_r):d\in D\}}\subset K^r.

It is invariant under every diagonal operator Δ(d)=diag⁡(d,…,d)\Delta(d)=\operatorname{diag}(d,\ldots,d), by multiplication in DD. It is reducing, since d∗∈Dd^*\in D. Its orthogonal projection QQ therefore commutes with each Δ(d)\Delta(d), by H01.

Let Rj:K→KrR_j:K\to K^r be the coordinate inclusion. The entries Qij=Ri∗QRjQ_{ij}=R_i^*QR_j are bounded operators, and the equation QΔ(d)=Δ(d)QQ\Delta(d)=\Delta(d)Q says Qijd=dQijQ_{ij}d=dQ_{ij}. Hence every QijQ_{ij} lies in D′D'. Since T∈D′′T\in D'', it commutes with every QijQ_{ij}, and therefore Δ(T)Q=QΔ(T)\Delta(T)Q=Q\Delta(T). Equation (ODF2) puts ξ\boldsymbol\xi in LL. It follows that

Δ(T)ξ=Δ(T)Qξ=QΔ(T)ξ∈L.\Delta(T)\boldsymbol\xi =\Delta(T)Q\boldsymbol\xi =Q\Delta(T)\boldsymbol\xi\in L.

The definition of LL now provides one d=π(a)d=\pi(a) satisfying (ODF3).

Conversely, D′′D'' is strongly closed and contains DD. Indeed, for b∈D′b\in D', the equation Sib=bSiS_ib=bS_i passes to a strong limit, since both evaluations use fixed vectors. Thus every strong limit from DD belongs to D′′D''. The two inclusions prove the theorem. □\square

The indices consisting of a finite vector set and a positive error, ordered by enlarging the set and decreasing the error, give a directed set. Choosing one approximant for each such index turns (ODF3) into a strong-convergent net. No countable cofinal family is required.

Finite-vector bicommutant approximation The tuple xi lies in the closed diagonal orbit L. The projection Q onto L commutes with the diagonal operator T because all entries of Q lie in the commutant D prime. Thus the image tuple T xi lies in L and can be approximated by one diagonal action d xi. xi = (xi_1, ..., xi_r) xi belongs to L approximate identity: ODF02 Delta(T) Delta(T) xi belongs to L Q_ij in D'; T in D'' Delta(T) Q = Q Delta(T) L = closure of {(d xi_1, ..., d xi_r) : d in D} One d approximates the entire image tuple: inequality (ODF3).

Figure. The maps Δ(d),Δ(T):Kr→Kr\Delta(d),\Delta(T):K^r\to K^r and Q:Kr→L⊂KrQ:K^r\to L\subset K^r are the actual operators in the ODF03 proof. The diagram depicts their invariant-subspace mechanism; it asserts no finite-dimensionality of KK or LL.

ODF04. Self-adjoint strong density by real separation

Lemma. Every y=y∗∈My=y^*\in M is a strong limit of operators π(ai)\pi(a_i) with ai=ai∗∈Aa_i=a_i^*\in A. Their norms are not asserted bounded.

Proof. ODF03 supplies a net di∈Dd_i\in D converging strongly to yy. Strong convergence implies weak operator convergence. The adjoints converge weakly to yy, because

⟨η,di∗ξ⟩=⟨ξ,diη⟩‾⟶⟨ξ,yη⟩‾=⟨η,yξ⟩.\langle\eta,d_i^*\xi\rangle =\overline{\langle\xi,d_i\eta\rangle} \longrightarrow\overline{\langle\xi,y\eta\rangle} =\langle\eta,y\xi\rangle.

Thus hi=(di+di∗)/2h_i=(d_i+d_i^*)/2 converges weakly to yy. Each hih_i has a self-adjoint lift (ai+ai∗)/2(a_i+a_i^*)/2 in AA.

Fix ξ1,…,ξr\xi_1,\ldots,\xi_r. The real linear map

Φ(h)=(hξ1,…,hξr)\Phi(h)=(h\xi_1,\ldots,h\xi_r)

takes the real vector space DhD_h into the real Hilbert space underlying KrK^r. Every continuous real linear functional on that Hilbert space has the form Re⁡∑j⟨ηj,vj⟩\operatorname{Re}\sum_j\langle\eta_j,v_j\rangle. To see this from H00, if ℓ\ell is real linear, then F(v)=ℓ(v)−iℓ(iv)F(v)=\ell(v)-i\ell(iv) is bounded complex linear and has a Hilbert representative; taking its real part recovers ℓ\ell.

The weak operator convergence just proved therefore puts Φ(y)\Phi(y) in the Banach weak closure of Φ(Dh)\Phi(D_h). This image is a real linear subspace, hence convex. The real separation proof SEP says that its weak and norm closures agree. Choose h∈Dhh\in D_h with ∑j∥(h−y)ξj∥2<ε2\sum_j\|(h-y)\xi_j\|^2<\varepsilon^2. Directing these choices by finite sets and errors proves strong density. □\square

ODF05. The rational contraction cutoff

Resolvent lemma. If bi=bi∗→y=y∗b_i=b_i^*\to y=y^* strongly, then

(bi−i1K)−1⟶(y−i1K)−1,(bi+i1K)−1⟶(y+i1K)−1(b_i-i1_K)^{-1}\longrightarrow(y-i1_K)^{-1},\qquad (b_i+i1_K)^{-1}\longrightarrow(y+i1_K)^{-1}

strongly, even when the ∥bi∥\|b_i\| have no uniform bound.

Proof. For a self-adjoint bounded operator bb,

∥(b±i1K)ξ∥2=∥bξ∥2+∥ξ∥2.\|(b\pm i1_K)\xi\|^2=\|b\xi\|^2+\|\xi\|^2.

The operator has closed range and zero kernel. Its adjoint b∓i1Kb\mp i1_K has zero kernel too, so that range is dense and therefore all of KK. Its inverse has norm at most one. The elementary inverse identity gives, for z=iz=i or z=−iz=-i,

(bi−z)−1−(y−z)−1=(bi−z)−1(y−bi)(y−z)−1.(b_i-z)^{-1}-(y-z)^{-1} =(b_i-z)^{-1}(y-b_i)(y-z)^{-1}.

For a fixed ξ\xi, the norm of the right side applied to ξ\xi is at most ∥(y−bi)(y−z)−1ξ∥→0\|(y-b_i)(y-z)^{-1}\xi\|\to0. The rightmost vector is fixed; the leftmost inverse has its own uniform bound. This proves the lemma without estimating ∥bi∥\|b_i\|. □\square

Put

f(t)=2t1+t2=1t−i+1t+i(t∈R).(ODF4)f(t)=\frac{2t}{1+t^2} =\frac1{t-i}+\frac1{t+i}\quad(t\in\mathbb R). \tag{ODF4}

It is real, f(0)=0f(0)=0, and ∣f(t)∣≤1|f(t)|\le1, since 2∣t∣≤1+t22|t|\le1+t^2. F06 gives f(a)∈Ahf(a)\in A_h with ∥f(a)∥≤1\|f(a)\|\le1 for every a=a∗∈Aa=a^*\in A. This assertion uses the forced unitization when necessary, and the vanishing value at zero puts the result back in AA. The resolvent lemma and (ODF4) give f(bi)→f(y)f(b_i)\to f(y) strongly.

Theorem (self-adjoint contraction density). Every h=h∗∈Mh=h^*\in M with ∥h∥≤1\|h\|\le1 is a strong* limit of π(ai)\pi(a_i), where ai=ai∗∈Aa_i=a_i^*\in A and ∥ai∥≤1\|a_i\|\le1.

Proof. If K=0K=0, take the constant zero net. Otherwise, in B(K)B(K), put

s=(1K−h2)1/2,y=h(1K+s)−1.s=(1_K-h^2)^{1/2},\qquad y=h(1_K+s)^{-1}.

These operators belong to MM, by its C*-calculus and inverse calculus. They commute, and y=y∗y=y^*. Indeed ss is obtained by continuous functions of h2h^2, and 1K+s≥1K1_K+s\ge1_K is invertible. The identity h2=1K−s2h^2=1_K-s^2 gives

1K+y2=((1K+s)2+h2)(1K+s)−2=2(1K+s)−1.1_K+y^2 =\big((1_K+s)^2+h^2\big)(1_K+s)^{-2} =2(1_K+s)^{-1}.

Consequently f(y)=2y(1K+y2)−1=hf(y)=2y(1_K+y^2)^{-1}=h. This includes ∥h∥=1\|h\|=1.

ODF04 supplies self-adjoint lifts ci∈Ahc_i\in A_h with π(ci)→y\pi(c_i)\to y strongly. Take ai=f(ci)a_i=f(c_i). The scalar bound gives ∥ai∥≤1\|a_i\|\le1 in AA, not just in its represented image. Extending π\pi to the forced unitization on KK sends the new unit to 1K1_K. The extension is a unital *-homomorphism, so it preserves inverses and the rational identity (ODF4); hence

π(ai)=f(π(ci))⟶f(y)=h.\pi(a_i)=f(\pi(c_i))\longrightarrow f(y)=h.

All these operators are self-adjoint, so this is strong* convergence. □\square

ODF06. Positive matrices with the same norm bound

Theorem (positive matrix Kaplansky density). For every n≥1n\ge1 and every X∈Mn(M)+X\in M_n(M)_+, there is a net Ci∈Mn(A)+C_i\in M_n(A)_+ such that

∥Ci∥≤∥X∥,π(n)(Ci)⟶Xstrongly* and ultraweakly on Kn.(ODF5)\|C_i\|\le\|X\|,\qquad \pi^{(n)}(C_i)\longrightarrow X \quad\hbox{strongly* and ultraweakly on }K^n. \tag{ODF5}

The same convergences hold after extension by zero to HnH^n.

Proof. First identify the strongly generated algebra of π(n)(Mn(A))\pi^{(n)}(M_n(A)). Its elements have entries in DD. The algebra Mn(M)M_n(M) is strongly closed: a strong limit has entries extracted by the coordinate inclusions and projections, and each limiting entry belongs to MM. It contains Mn(D)M_n(D).

Conversely, let Z=[zpq]∈Mn(M)Z=[z_{pq}]\in M_n(M), and fix finitely many vectors in KnK^n. For each entry zpqz_{pq}, ODF03 supplies an element of DD approximating that entry on all the finitely many qq-th vector components. If each entry error on each component is less than ε/(nn)\varepsilon/(n\sqrt n), each output row error is less than ε/n\varepsilon/\sqrt n, and the full output vector error is less than ε\varepsilon. Thus Mn(D)M_n(D) is strongly dense in Mn(M)M_n(M). Its essential space is KnK^n: diagonal copies of π(eλ)\pi(e_\lambda) converge strongly to 1Kn1_{K^n}. Applying ODF03 to the representation π(n)\pi^{(n)} identifies its bicommutant with Mn(M)M_n(M).

If X=0X=0, take the constant zero net. Otherwise put c=∥X∥>0c=\|X\|>0, and let Z=(X/c)1/2∈Mn(M)Z=(X/c)^{1/2}\in M_n(M). It is a self-adjoint contraction. Apply ODF05 to the C*-algebra Mn(A)M_n(A) and its representation π(n)\pi^{(n)}. We obtain self-adjoint Bi∈Mn(A)B_i\in M_n(A), ∥Bi∥≤1\|B_i\|\le1, with π(n)(Bi)→Z\pi^{(n)}(B_i)\to Z strongly. Set

Ci=cBi2.C_i=cB_i^2.

These matrices are positive and satisfy ∥Ci∥≤c\|C_i\|\le c. ODF01's bounded product estimate gives π(n)(Ci)→cZ2=X\pi^{(n)}(C_i)\to cZ^2=X strongly. The matrices and the target are self-adjoint, so convergence is strong*. Their represented norms are bounded by cc, and ODF01 then gives ultraweak convergence.

For extension by zero, a vector of HnH^n is tested only through its orthogonal projection onto KnK^n. This proves strong and strong* convergence on HnH^n; the same norm bound and ODF01 give ultraweak convergence there. □\square

In particular the positive part of the unit ball of a faithfully represented C*-algebra is strongly and ultraweakly dense in the positive unit ball of its generated von Neumann algebra. The statement for Choi matrices uses (ODF5) with that same finite matrix size.

ODF07. The entire contraction ball and the closure algebra

Every contraction T∈MT\in M is a strong* limit of π(ai)\pi(a_i) with ∥ai∥≤1\|a_i\|\le1. To prove this, the self-adjoint matrix

Y=(0TT∗0)∈M2(M)Y=\begin{pmatrix}0&T\\T^*&0\end{pmatrix}\in M_2(M)

has norm ∥T∥\|T\|. Its square is diag⁡(TT∗,T∗T)\operatorname{diag}(TT^*,T^*T), and the C*-identity and the norm of a block diagonal operator prove this equality. Apply ODF05 at matrix size two to obtain self-adjoint contractions

Bi=(biaiai∗di)∈M2(A),π(2)(Bi)⟶Ystrongly.B_i=\begin{pmatrix}b_i&a_i\\a_i^*&d_i\end{pmatrix}\in M_2(A), \qquad\pi^{(2)}(B_i)\longrightarrow Y\quad\hbox{strongly}.

The matrix norm inequality ∥ai∥≤∥Bi∥≤1\|a_i\|\le\|B_i\|\le1 is part of the matrix construction linked above. The two off-diagonal corners give π(ai)→T\pi(a_i)\to T and π(ai)∗→T∗\pi(a_i)^*\to T^* strongly. This proves the assertion. The uniformly bounded approximants also converge ultraweakly, by ODF01.

It follows that the strong, strong* and ultraweak closures of DD, extended by zero on K⊥K^\perp, all equal the supported algebra MM. For the reverse inclusion in the ultraweak closure, D′′D'' on KK is ultraweakly closed: for each b∈D′b\in D', the equations ⟨η,(Tb−bT)ξ⟩=0\langle\eta,(Tb-bT)\xi\rangle=0 are differences of one-term functionals (ODF1). On HH, the additional equations T=PTPT=PTP are also ultraweakly closed by the same one-term tests. The strong* and strong reverse inclusions follow from their fixed-vector versions. On a nondegenerate representation K=HK=H, so each closure is precisely π(A)′′\pi(A)''.

References

The bicommutant theorem is due to John von Neumann. The finite-vector projection argument and the rational cutoff above give its density consequence and Kaplansky's theorem at the hypotheses stated here.

Irving Kaplansky, A theorem on rings of operators, Pacific Journal of Mathematics 1 (1951), 227–232. Theorem 1, printed pp.227–231, is the bounded density theorem; Lemmas 1–5, printed pp.228–230, develop the bounded-calculus and Cayley-resolvent method. The real separation, finite amplification and nonunital support arguments needed in this lesson are proved above from the linked programme foundations.