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LEVEL 3 OF 3 · The strong Kadison–Kastler conjecture
Close Separable C*-Algebras Without Spatial Conjugacy
expertly designed by an internal OpenAI model · released 2026-10-05
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IntroductionFor \(C^*\)-algebras \(A,B\subseteq\mathcal B(H)\), write \(A_1\) and \(B_1\) for their closed unit balls. Their Kadison–Kastler distance is \[ d_{\mathrm{KK}}(A,B)=\max\left\{ \sup_{a\in A_1}\inf_{b\in B_1}\left\|a-b\right\|,\, \sup_{b\in B_1}\inf_{a\in A_1}\left\|b-a\right\|\right\}. \tag{1}\] The spatial form of the perturbation problem asks whether sufficiently close algebras must be related by \(uAu^*=B\) for a unitary \(u\in\mathcal B(H)\). Kadison and Kastler initiated this problem in [6]. In its separable \(C^*\)-algebraic form, one asks for a constant \(\delta>0\) valid for all norm-separable \(C^*\)-algebras on separable Hilbert spaces; no bound on \(\left\|u-I\right\|\) is required. The following theorem resolves negatively this separable \(C^*\)-algebraic spatial form of the Kadison–Kastler conjecture, even for unital algebras with a common identity. Theorem 1. For every \(\varepsilon>0\) there are a separable complex Hilbert space \(H\) and unital, norm-separable \(C^*\)-algebras \(A,B\subseteq\mathcal B(H)\) with common identity \(I_H\) such that \[d_{\mathrm{KK}}(A,B)<\varepsilon,\qquad A''=B'',\] but no unitary \(u\in\mathcal B(H)\) satisfies \(uAu^*=B\). The scope of this statement is important. Johnson constructed arbitrarily close separable nuclear algebras for which implementing unitaries cannot be chosen close to the identity [5]; those examples are nevertheless spatially conjugate. Choi and Christensen constructed arbitrarily close nonisomorphic algebras [2], but norm nonseparability is essential to those examples. These distinctions, and the resulting separable spatial formulation, are discussed in [3]. In the positive direction, Christensen, Sinclair, Smith, White, and Winter proved spatial conjugacy for sufficiently close separable nuclear \(C^*\)-algebras on a separable Hilbert space [3]; see [4] for the full proof. Theorem 1 imposes no nuclearity assumption. It makes no assertion of abstract nonisomorphism and does not give a counterexample for von Neumann algebras. The construction.We first isolate a way to turn an obstruction for inclusions into an obstruction to arbitrary spatial conjugacy. Let \(D\subseteq\mathcal B(L)\) be unital, norm-separable, and have scalar center. For unital subalgebras \(P,Q\subseteq D\), consider the algebra \[\mathcal E_D(P)=\{(x_n):x_n\in D,\ x_n\longrightarrow p\in P \text{ in norm}\}\] acting diagonally on \(\bigoplus_{n\ge1}L\). Changing \(P\) changes only the condition at the limit. The coordinate projections are intrinsic minimal central projections of this algebra. Consequently, a unitary conjugating \(\mathcal E_D(P)\) onto \(\mathcal E_D(Q)\) must permute the coordinates and normalize \(D\) on every coordinate. Pulling back constant sequences then forces each finite family in \(Q\) to be a simultaneous norm limit of families in unitary conjugates of \(P\) by normalizers of \(D\). Write \(D'\) for the commutant of \(D\) on \(L\), consisting of the bounded operators commuting with every element of \(D\). The obstruction we use is the equality \[ \left\|\sum_i p_i z_i\right\|_{\mathcal B(L)} =\left\|\sum_i p_i\otimes z_i\right\|_{\mathcal B(L\otimes L)}, \qquad p_i\in P,\quad z_i\in D'. \tag{2}\] This equality is invariant under normalizers of \(D\) and passes to simultaneous finite-family norm limits. We construct very close subalgebras \(P_0,P_t\subseteq D\) for which it holds for \(P_0\) but fails for \(P_t\). In fact, \(P_0\) and \(P_t\) themselves are conjugate by a unitary close to the identity. The obstruction concerns their positions inside \(D\), and the sequence construction makes it an obstruction to every spatial conjugacy of the resulting algebras. For the close inclusions we use a real-parameter deformation of the regular representation of the free group on countably many generators. This representation-theoretic ingredient belongs to the Pytlik–Szwarc family [7]; its uniform-topology behavior at the regular representation is discussed by Burger, Ozawa, and Thom [1]. We give a direct tree construction and prove the uniform estimate needed here. The additional mechanism is the combination of the relative tensor-norm test with the convergent-sequence reduction. The reduction is stated separately, so it can be used for other pairs of inclusions. Section 2 proves the reduction. Section 3 constructs the representations, and Section 4 establishes the tensor-norm obstruction. Section 5 assembles the counterexamples. All Hilbert spaces are complex, and all operator tensor products below act on the indicated Hilbert-space tensor products. No abstract choice of \(C^*\)-tensor norm is needed. Unital subalgebras are understood to contain the identity of their ambient operator algebra. A convergent-sequence obstructionWe explain how the limit condition records an inclusion \(P\subseteq D\). The resulting algebras preserve the distance between limit algebras, but their spatial conjugacies are constrained by the coordinate algebra \(D\). Proposition 2. Let \(L\) be a nonzero separable Hilbert space, let \(D\subseteq\mathcal B(L)\) be a unital norm-separable \(C^*\)-algebra with \(Z(D)=\mathbb CI_L\), and let \(P,Q\subseteq D\) be unital \(C^*\)-subalgebras containing \(I_L\). On \(H=\bigoplus_{n\ge1}L\), define \[ \mathcal E_D(P)=\{(x_n)_{n\ge1}:x_n\in D,\ x_n\to p\in P\text{ in norm}\}, \tag{3}\] and define \(\mathcal E_D(Q)\) similarly. Then:
Proof. A norm-convergent sequence is bounded, so (3) defines a diagonal operator on \(H\), with norm \(\sup_n\left\|x_n\right\|\). Algebra operations and adjoints preserve the limit condition, and the constant identity belongs to the algebra. To check norm closedness, suppose \(x^{(k)}\to x\) in the supremum norm, with coordinate limits \(p_k\in P\). Then \[\left\|p_k-p_j\right\|\le\sup_n\left\|x_n^{(k)}-x_n^{(j)}\right\|.\] Thus \(p_k\to p\in P\). The estimate \[\left\|x_n-p\right\|\le\left\|x_n-x_n^{(k)}\right\| +\left\|x_n^{(k)}-p_k\right\|+\left\|p_k-p\right\|\] shows that \(x_n\to p\). Moreover, \[ \mathcal E_D(P)=c_0(\mathbb N,D)+\{(p,p,\ldots):p\in P\}. \tag{6}\] The two summands are norm-separable: \(P\) is a subspace of the separable metric space \(D\), and finite-support sequences from a countable dense subset of \(D\) are dense in \(c_0(\mathbb N,D)\). Their sum is norm-separable. For the metric assertion, write \(\alpha(P,Q)=\sup_{p\in P_1}\mathop{\mathrm{dist}}(p,Q_1)\). Given a contraction \(x\in\mathcal E_D(P)\) with limit \(p\) and \(\eta>0\), choose \(q\in Q_1\) with \(\left\|p-q\right\|<\alpha(P,Q)+\eta\), and choose \(N\) so that \(\sup_{n>N}\left\|x_n-p\right\|<\eta\). Keeping the first \(N\) entries of \(x\) and putting \(q\) thereafter gives a contraction \(y\in\mathcal E_D(Q)\) with \(\left\|x-y\right\|<\alpha(P,Q)+2\eta\). This proves the upper bound for the directed distance. Conversely, for a constant contraction \((p,p,\ldots)\) and any contraction \(y\in\mathcal E_D(Q)\) with limit \(q\in Q_1\), \[\left\|(p,p,\ldots)-y\right\|=\sup_n\left\|p-y_n\right\|\ge\left\|p-q\right\| \ge\mathop{\mathrm{dist}}(p,Q_1).\] Taking infima and suprema proves equality of the directed distances. Interchanging \(P,Q\) gives (4). Let \(e_n\) be the projection onto the \(n\)th copy of \(L\). Every \(e_n\) is a central element of \(\mathcal E_D(P)\). Conversely, a central element \((x_n)\) commutes with all finite-support \(D\)-valued sequences, so each \(x_n\) lies in \(Z(D)=\mathbb CI_L\). Thus the center consists exactly of convergent scalar sequences. Every nonzero central projection contains an \(e_n\), and hence the minimal nonzero central projections are precisely the \(e_n\). The same holds for \(\mathcal E_D(Q)\). If \(S\mathcal E_D(P)S^*=\mathcal E_D(Q)\), conjugation by \(S\) therefore permutes the projections \(e_n\). Its restriction from the \(n\)th coordinate to its image is a unitary \(U_n:L\to L\). The corresponding coordinate corners of both algebras are exactly \(D\), since every finitely supported \(D\)-valued sequence is allowed. Consequently \(U_nDU_n^*=D\). For \(b\in Q\), pull back the constant sequence \((b,b,\ldots)\) under \(S\). Its \(n\)th entry is \(U_n^*bU_n\), regardless of the coordinate permutation. It belongs to \(\mathcal E_D(P)\), so its entries converge in norm to some \(p_b\in P\). This is equivalent to (5) and proves (ii). Finally, an operator commuting with \(\mathcal E_D(P)\) commutes with all \(e_n\), so it is block diagonal. Commutation with the finite-support \(D\) corners means that each block lies in \(D'\). These conditions are also sufficient, and do not depend on \(P\). Thus both commutants equal \[\{(z_n):z_n\in D',\ \sup_n\left\|z_n\right\|<\infty\}.\] This proves (iii). ◻ We next give a concrete condition preserved by the approximation in Proposition 2(ii). Definition 3. For a unital inclusion \(P\subseteq D\subseteq\mathcal B(L)\), say that \(P\) has the spatial tensor-norm identity relative to \(D\) if \[ \left\|\sum_{i=1}^m p_i z_i\right\|_{\mathcal B(L)} =\left\|\sum_{i=1}^m p_i\otimes z_i\right\|_{\mathcal B(L\otimes L)} \tag{7}\] for every positive integer \(m\), all \(p_1,\ldots,p_m\in P\), and all \(z_1,\ldots,z_m\in D'\). Lemma 4. Let \(P,Q\subseteq D\subseteq\mathcal B(L)\) be unital \(C^*\)-algebras. The identity in Definition 3 is preserved by conjugating \(P\) with any unitary normalizing \(D\). If \((U_n)\) is a sequence of unitaries in \(\mathcal B(L)\) satisfying \(U_nDU_n^*=D\) and every \(b\in Q\) admits the approximation (5), then the identity for \(P\) implies the identity for \(Q\). Proof. If \(UDU^*=D\), then \(UD'U^*=D'\). For \(q_i=Up_iU^*\) and \(z_i\in D'\), apply (7) to \(p_i\) and \(U^*z_iU\). Conjugate its product sum by \(U\) and its tensor sum by \(U\otimes U\). This gives (7) for \(q_i,z_i\). Now fix finite families \(b_i\in Q\) and \(z_i\in D'\). Put \(q_{i,n}=U_np_{b_i}U_n^*\). For each \(n\), the first part gives the identity for the entire list \((q_{i,n})_i\), since its entries all lie in \(U_nPU_n^*\). Both errors \[\left\|\sum_i(q_{i,n}-b_i)z_i\right\|,\qquad \left\|\sum_i(q_{i,n}-b_i)\otimes z_i\right\|\] are at most \(\sum_i\left\|q_{i,n}-b_i\right\|\left\|z_i\right\|\), which tends to zero. Taking the limit proves the identity for the prescribed families in \(Q\) and \(D'\). ◻ Corollary 5. Under the hypotheses of Proposition 2, suppose that \(P\) has the spatial tensor-norm identity relative to \(D\), whereas \(Q\) does not. Then \(\mathcal E_D(P)\) and \(\mathcal E_D(Q)\) are not spatially conjugate. If \(W\in\mathcal B(L)\) is unitary and \(WPW^*=Q\), then nevertheless \[d_{\mathrm{KK}}(\mathcal E_D(P),\mathcal E_D(Q))\le2\left\|W-I_L\right\|.\] Proof. A spatial conjugacy would give the unitaries in Proposition 2(ii), contradicting Lemma 4. For the distance bound, \(p\mapsto WpW^*\) bijects the closed unit balls and \[\left\|WpW^*-p\right\|\le2\left\|p\right\|\left\|W-I_L\right\|.\] Apply Proposition 2(i). ◻ The unitary \(W\) used for the distance estimate is not required to normalize \(D\). Indeed, under the stated tensor-norm obstruction, no unitary normalizing \(D\) can conjugate \(P\) onto \(Q\). A uniformly small free-group deformationWe now construct the representations used to produce the inclusions in Corollary 5. Let \(G\) be the free group on the countable set \(\{s_1,s_2,\ldots\}\), let \(e\) denote its identity, and put \(K=\ell^2(G)\). On its usual orthonormal basis define \[ \lambda(g)\delta_x=\delta_{gx},\qquad \rho(g)\delta_x=\delta_{xg^{-1}}. \tag{8}\] Both are unitary representations, and every left translation commutes with every right translation. The group \(G\) is countable, so \(K\) is separable. The following elementary version of the real Pytlik–Szwarc deformation [7, 1] records exactly the coefficient and uniform estimate that the proof needs. Lemma 6. For every \(0<t<1\), there is a unitary representation \(\pi_t:G\to\mathcal B(K)\) such that, with \(r=\sqrt{1-t^2}\), \[\begin{align*} \left\langle \pi_t(s_i)\delta_e,\delta_e\right\rangle&=t\quad(i\ge1),\tag{9}\\ \sup_{g\in G}\left\|\pi_t(g)-\lambda(g)\right\|&\le c(t),\qquad c(t)=2(1-r)+\frac{t}{1-t}+t. \tag{10}\end{align*}\] In particular, \(c(t)\to0\) as \(t\downarrow0\). Proof. Use the tree of reduced words with edges given by right multiplication by a generator or its inverse, rooted at \(e\). Its distance is \(d(x,y)=|x^{-1}y|\), so left translations preserve distance. For \(x\ne e\), let \(p(x)\) be the neighbor of \(x\) toward \(e\), obtained by deleting the last letter of its reduced word. Recursively define \[ \xi_e=\delta_e,\qquad \xi_x=t\xi_{p(x)}+r\delta_x\quad(x\ne e). \tag{11}\] These are unit vectors supported on their root paths. If \(z\) is the last common vertex of the root paths to \(x\) and \(y\), the common-support components are \(t^{d(x,z)}\xi_z\) and \(t^{d(y,z)}\xi_z\), respectively. The remaining supports are disjoint. Hence \[ \left\langle \xi_x,\xi_y\right\rangle=t^{d(x,y)}. \tag{12}\] Also \(\delta_e=\xi_e\) and \(\delta_x=(\xi_x-t\xi_{p(x)})/r\) for \(x\ne e\), so their span is dense. The assignment \(\xi_x\mapsto\xi_{gx}\) preserves every finite Gram matrix by (12). It therefore defines an isometry on the span, and the inverse assignment for \(g^{-1}\) makes the extension unitary. Denote this unitary by \(\pi_t(g)\). The representation law holds on the dense span and hence on \(K\). Since \(\pi_t(s_i)\delta_e=\xi_{s_i}=t\delta_e+r\delta_{s_i}\), (9) follows. It remains to prove that the perturbation is uniformly small over all group elements, rather than just over the generators. Fix \(g\ne e\), write \(h_0=e,h_1,\ldots,h_l=g\) for its root path, and put \(T=\pi_t(g)\lambda(g)^*\). For \(y\ne g\), (11) gives \[ T\delta_y=\frac{\xi_y-t\xi_{g p(g^{-1}y)}}{r}. \tag{13}\] The vertex \(g p(g^{-1}y)\) is the neighbor of \(y\) toward \(g\). If \(y\) is off the path \([e,g]\), this neighbor is also \(p(y)\), the neighbor toward \(e\); see Figure 1. Thus \(T\delta_y=\delta_y\) off that path. On the path, the neighbor toward \(g\) of \(h_k\), for \(k<l\), is \(h_{k+1}\), so \[ T\delta_{h_k}=r\xi_{h_k}-t\delta_{h_{k+1}}\quad(0\le k<l), \qquad T\delta_{h_l}=\xi_{h_l}. \tag{14}\] Let \(M_g=\mathop{\mathrm{span}}\{\delta_{h_k}:0\le k\le l\}\). On this space define the truncated shift \(S\delta_{h_k}=\delta_{h_{k+1}}\) for \(k<l\) and \(S\delta_{h_l}=0\), and put \(X\delta_{h_k}=\xi_{h_k}\). For \(R=\operatorname{diag}(1,r,\ldots,r)\), the recursion gives \[ X=R(I-tS^*)^{-1}. \tag{15}\] Indeed, its \(k\)th column is \(t^k\delta_e+r\sum_{j=1}^k t^{k-j}\delta_{h_j}\). Since \(\left\|S\right\|\le1\) and \(\left\|R\right\|=1\), \[ \left\|X-I\right\|\le\left\|R-I\right\| +\left\|R\right\|\sum_{j=1}^{\infty}t^j \le1-r+\frac{t}{1-t}. \tag{16}\] Writing \(R'=\operatorname{diag}(r,\ldots,r,1)\), (14) becomes \(T|_{M_g}=XR'-tS\). Therefore \[\begin{align*} \left\|T|_{M_g}-I\right\| &\le\left\|(X-I)R'\right\|+\left\|R'-I\right\|+t\left\|S\right\|\\ &\le2(1-r)+\frac{t}{1-t}+t=c(t). \end{align*}\] The same bound holds on \(K\), since \(T\) is the identity on \(M_g^\perp\). Multiplication by \(\lambda(g)\) proves (10). For \(g=e\) the difference is zero, so the supremum includes this case as well. ◻ Remark 7. Only the operator \(X\) on a single finite path is used in the estimate. On this infinitely branching tree, the global map \(\delta_x\mapsto\xi_x\) need not be bounded: the vectors \(\xi_{s_i}\) all have root coefficient \(t\). The Gram-matrix construction of \(\pi_t\) does not require such a global bounded map. Close inclusions distinguished by a tensor normFix \(0<t<1\), let \(\pi_t\) be given by Lemma 6, and write \(\pi_0=\lambda\). We construct a common coordinate algebra \(D\) and subalgebras \(P_0,P_t\) satisfying Corollary 5. First we record the absorption calculation that will be used both for closeness and for the tensor-norm estimate. Lemma 8 (Absorption). Let \(\sigma\) be a unitary representation of \(G\) on a nonzero Hilbert space \(J\). The operator \[W_\sigma(\delta_x\otimes v)=\delta_x\otimes\sigma(x)v \quad(x\in G,\ v\in J)\] is unitary on \(K\otimes J\) and satisfies \[ W_\sigma(\lambda(g)\otimes I_J)W_\sigma^* =\lambda(g)\otimes\sigma(g)\quad(g\in G). \tag{17}\] Proof. The operator is the orthogonal direct sum of the unitaries \(\sigma(x)\). On \(\delta_x\otimes v\), the left side of (17) equals \[\delta_{gx}\otimes\sigma(gx)\sigma(x)^*v =\delta_{gx}\otimes\sigma(g)v. \qedhere\] ◻ On \(L=K\otimes K\), put \[ Q_a(g)=\lambda(g)\otimes\pi_a(g),\qquad P_a=C^*(Q_a(g):g\in G)\quad(a=0,t). \tag{18}\] For the matrix units \(E_{xy}\delta_z=\mathbf1_{\{z=y\}}\delta_x\) on \(K\), define \(D\subseteq\mathcal B(L)\) to be generated by \[ \lambda(g)\otimes I_K,\quad I_K\otimes\pi_0(g),\quad I_K\otimes\pi_t(g)\quad(g\in G), \qquad I_K\otimes E_{xy}\quad(x,y\in G). \tag{19}\] The generators include the identity, and \(P_0,P_t\subseteq D\). All three algebras are norm-separable, since their generating sets are countable. Lemma 9. The algebra \(D\) in (19) has scalar center, and \[ D'=\{Y\otimes I_K:Y\in\lambda(G)'\}. \tag{20}\] There is a unitary \(W\in\mathcal B(L)\) such that \[ WP_0W^*=P_t,\qquad \left\|W-I_L\right\|\le c(t). \tag{21}\] Proof. Commutation with all \(I_K\otimes E_{xy}\) forces a bounded operator to be \(Y\otimes I_K\): commutation with the diagonal matrix units removes off-diagonal blocks, and commutation with the remaining units makes the diagonal blocks identical. The first-factor generators then impose exactly \(Y\in\lambda(G)'\). Such operators commute with all the second-factor generators, proving (20). In particular, \(\rho(g)\otimes I_K\in D'\). If \(Y\otimes I_K\in Z(D)\), then \(Y\) commutes with \(\lambda(G)\) by (20). It also commutes with \(\rho(G)\), since \(Y\otimes I_K\) belongs to \(D\) and the right translations belong to \(D'\). Thus \(Y\delta_e\) is invariant under \(\lambda(g)\rho(g)\), which acts on the basis by conjugation \(x\mapsto gxg^{-1}\). Every nonidentity conjugacy class in \(G\) is infinite: conjugate a fixed nonidentity reduced word by distinct generators absent from that word. A square-summable vector invariant under conjugation must therefore be supported at \(e\). Write \(Y\delta_e=\alpha\delta_e\). Commuting with left translations gives \(Y\delta_x=\alpha\delta_x\) for every \(x\), proving \(Z(D)=\mathbb CI_L\). For the final assertion, Lemma 8 shows that \(W=W_{\pi_t}W_{\pi_0}^*\) sends every \(Q_0(g)\) to \(Q_t(g)\) by conjugation. Moreover, the direct-sum description of these unitaries gives \[\left\|W-I_L\right\|=\left\|W_{\pi_t}-W_{\pi_0}\right\| =\sup_{x\in G}\left\|\pi_t(x)-\lambda(x)\right\|\le c(t). \qedhere\] ◻ Lemma 10. The inclusion \(P_0\subseteq D\) has the spatial tensor-norm identity. Proof. Define a unitary on \(L\) by \[V(v\otimes\delta_x)=\lambda(x)^*v\otimes\delta_x.\] It commutes with every element of \(D'\) by (20). On elementary vectors one computes \[VQ_0(g)V^*(v\otimes\delta_x)=v\otimes\delta_{gx}.\] Thus \(VP_0V^*=I_K\otimes C^*(\lambda(G))\). Given finite families \(p_i\in P_0\) and \(z_i\in D'\), write \[Vp_iV^*=I_K\otimes X_i,\qquad z_i=Y_i\otimes I_K.\] Conjugation by \(V\) gives \[\left\|\sum_i p_i z_i\right\|=\left\|\sum_i Y_i\otimes X_i\right\|.\] On \(L\otimes L=K^{\otimes4}\), conjugation by \(V\otimes I_L\) gives \[\left\|\sum_i p_i\otimes z_i\right\| =\left\|\sum_iI_K\otimes X_i\otimes Y_i\otimes I_K\right\| =\left\|\sum_iY_i\otimes X_i\right\|.\] The last equality permutes the four tensor factors and uses the fact that tensoring with a nonzero identity operator does not change norm. This proves (7). ◻ For \(P_t\), the identity will fail because the product norm has a lower bound linear in the number of generators, while absorption gives a square-root upper bound on the tensor norm. Lemma 11. For every positive integer \(m\), \[ \left\|\sum_{i=1}^m\lambda(s_i)\right\|\le2\sqrt m. \tag{22}\] Proof. Let \(F_i\) be the orthogonal projection onto the closed span of words beginning with \(s_i^{-1}\). The \(F_i\) are pairwise orthogonal. Write \(\lambda(s_i)=A_i+B_i\), where \[A_i=\lambda(s_i)(I_K-F_i),\qquad B_i=\lambda(s_i)F_i.\] There is no cancellation when \(s_i\) is prepended to a word not beginning with \(s_i^{-1}\). Thus the range of \(A_i\) consists of vectors supported on words beginning with \(s_i\), and these ranges are mutually orthogonal. For every \(v\in K\), \[\left\|\sum_i A_iv\right\|^2=\sum_i\left\|(I_K-F_i)v\right\|^2 \le m\left\|v\right\|^2,\] while \[\left\|\sum_i B_iv\right\|\le\sum_i\left\|F_iv\right\| \le\sqrt m\left(\sum_i\left\|F_iv\right\|^2\right)^{1/2} \le\sqrt m\left\|v\right\|.\] Adding the two bounds proves (22). ◻ Lemma 12. For every \(0<t<1\), the inclusion \(P_t\subseteq D\) fails the spatial tensor-norm identity. Proof. Choose an integer \(m>4/t^2\), so \(mt>2\sqrt m\), and take \[p_i=Q_t(s_i),\qquad z_i=\rho(s_i)\otimes I_K, \qquad 1\le i\le m.\] These belong to \(P_t\) and \(D'\), respectively. Since \(\lambda(s_i)\rho(s_i)\delta_e=\delta_e\), (9) implies \[ \left\|\sum_i p_i z_i\right\| \ge\left|\left\langle \left(\sum_i p_i z_i\right) (\delta_e\otimes\delta_e),\delta_e\otimes\delta_e\right\rangle\right| =mt. \tag{23}\] On the other hand, the tensor sum on \(L\otimes L\) is \[\sum_{i=1}^m\lambda(s_i)\otimes\pi_t(s_i) \otimes\rho(s_i)\otimes I_K.\] Apply Lemma 8 to the representation \(\sigma=\pi_t\otimes\rho\otimes1\) on \(K^{\otimes3}\), where \(1\) is the trivial representation on the last copy of \(K\). Together with Lemma 11, it gives \[ \left\|\sum_i p_i\otimes z_i\right\| =\left\|\sum_{i=1}^m\lambda(s_i)\right\|\le2\sqrt m<mt. \tag{24}\] Equations (23) and (24) contradict the identity for this finite list. ◻ The counterexamplesProof of Theorem 1. Given \(\varepsilon>0\), choose \(0<t<1\) so small that \(2c(t)<\varepsilon\). Use the algebras \(P_0,P_t\subseteq D\subseteq\mathcal B(L)\) from Section 4, and put \[H=\bigoplus_{n\ge1}L,\qquad A=\mathcal E_D(P_0),\qquad B=\mathcal E_D(P_t).\] The space \(H\) is separable. Lemma 9 supplies the scalar center of \(D\), so Proposition 2 shows that \(A,B\) are unital norm-separable \(C^*\)-algebras with common identity and that \(A''=B''\). The same lemma supplies a unitary \(W\) with \(WP_0W^*=P_t\) and \(\left\|W-I_L\right\|\le c(t)\). By Corollary 5, \[d_{\mathrm{KK}}(A,B)\le2c(t)<\varepsilon.\] Finally, Lemmas 10 and 12 show that the relative tensor-norm identity holds for \(P_0\) but not for \(P_t\). Corollary 5 therefore excludes every unitary conjugating \(A\) onto \(B\). ◻ The common ideal \(c_0(\mathbb N,D)\) makes the von Neumann closures agree, while the norm-limit condition retains the distinction between the two inclusions.
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