Introduction

The Razak–Jacelon algebra W\mathcal{W} is a simple, monotracial, stably projectionless nuclear C∗C^*-algebra [21]. Tensoring by W\mathcal{W} removes the KK-theoretic part of the classification problem and makes the order on the Cuntz semigroup visible through traces. The question is whether the resulting trace data determine the algebra even when its ideal structure is unrestricted. We prove that they do.

The invariant and the main theorem

For a C∗C^*-algebra CC, let T(C)T(C) consist of all maps τ:C+→[0,∞]\tau:C_+\to[0,\infty] satisfying

τ(0)=0,τ(a+b)=τ(a)+τ(b),τ(ra)=rτ(a)(r>0),\tau(0)=0,\qquad\tau(a+b)=\tau(a)+\tau(b),\qquad\tau(ra)=r\tau(a)\quad(r>0),

together with τ(x∗x)=τ(xx∗)\tau(x^*x)=\tau(xx^*) and lower semicontinuity for norm-convergent nets in C+C_+. Arithmetic is extended nonnegative arithmetic. We impose no density condition on the finite domain. In particular, every closed two-sided ideal II contributes the weight

τI(a)={0,a∈I+,∞,a∈C+∖I+.\tau_I(a)=\begin{cases}0,&a\in I_+,\\ \infty,&a\in C_+\setminus I_+.\end{cases}

The canonical topology is specified by

τi⟶τ⟺lim sup⁡iτi((a−ε)+)≤τ(a)≤lim inf⁡iτi(a)(a∈C+, ε>0).(1)\tau_i\longrightarrow\tau\quad\Longleftrightarrow\quad\limsup_i\tau_i((a-\varepsilon)_+)\leq\tau(a)\leq\liminf_i\tau_i(a)\quad(a\in C_+,\ \varepsilon>0). \tag*{(1)}

An isomorphism of these topological cones is a homeomorphism preserving addition, the zero weight, and multiplication by every positive real scalar.

Theorem 1.1. Let AA and BB be separable nuclear complex C∗C^*-algebras. If T(A)T(A) and T(B)T(B) are isomorphic as topological cones, then

A⊗W⊗K≅B⊗W⊗K,A\otimes\mathcal{W}\otimes\mathcal{K}\cong B\otimes\mathcal{W}\otimes\mathcal{K},

where K=K(ℓ2(N))\mathcal{K}=\mathcal{K}(\ell^2(\mathbb{N})) and all tensor products are spatial.

The conclusion is an actual C∗C^*-algebra isomorphism. The algebras may be nonunital, may have both finite and infinite subquotients, and may have an arbitrary primitive ideal space. Their only regularity assumptions are separability and nuclearity. Moreover, the isomorphism can realize the prescribed cone map: after transporting the given map to F:T(B⊗W⊗K)→T(A⊗W⊗K)F:T(B\otimes\mathcal{W}\otimes\mathcal{K})\to T(A\otimes\mathcal{W}\otimes\mathcal{K}), we obtain an isomorphism Φ\Phi with τ∘Φ=F(τ)\tau\circ\Phi=F(\tau) for every extended trace τ\tau. This refinement is proved at the end of Theorem 8.5.

The presence of (1.1) makes the invariant sensitive to this ideal structure. For example,

I⊆J⟺τI+τJ=τI.I\subseteq J \quad\Longleftrightarrow\quad\tau_I+\tau_J=\tau_I.

The finite and zero ideals of a general weight are also encoded by the two limiting operations obtained by letting its positive scalar multiple tend to zero and to infinity. These features will let us localize each approximation on the ideal where its controlling trace is finite.

History and significance

Razak’s classification of simple inductive limits of stably projectionless building blocks made the cone of traces, together with its scale, an effective classification invariant [27]. Jacelon’s construction singled out the simple monotracial algebra W\mathcal{W} in this setting [21]. The existence, uniqueness, and approximate-intertwining organization of those classification arguments also provides the broad method used here, with new local estimates needed for arbitrary ideals.

The trace-cone question is due to Leonel Robert. It was recorded in Santiago’s 2012 conference abstract [30] and appears as Problem LXVIII in the survey of Schafhauser, Tikuisis, and White [32]. Their formulation retains every extended trace, including the zero/infinity ideal weights. Their May 2026 discussion describes the known simple and traceless cases and the difficulty already presented by one proper nonzero ideal. Theorem 1.1 gives a positive answer to that problem for the full cone and the unrestricted class of separable nuclear algebras in its statement.

Elliott, Robert, and Santiago developed the compact topological cone of extended lower-semicontinuous traces and its relation to functionals on the Cuntz semigroup [14]. Robert subsequently identified tensoring with W\mathcal{W} with realification of that semigroup [28]. Thus the cone in (1) determines the Cuntz semigroup of the stabilized algebra, including its ideals and positive real scalar multiplication. The remaining task is to realize this invariant by algebra maps and prove their uniqueness.

In the tracial simple case, the work of Elliott and Niu [13] and the published classification of Elliott, Gong, Lin, and Niu [12], Theorem 7.5 establish classification by scaled traces under the stated KKKK-contractibility and finite-nuclear-dimension hypotheses. Castillejos and Evington’s nuclear-dimension theorem for simple separable nuclear Z\mathcal{Z}-stable algebras supplies the regularity bridge for the simple stabilized case [3], Theorem A. Nawata gave another proof that A⊗W≅WA\otimes\mathcal{W}\cong\mathcal{W} when AA is simple, separable, nuclear, has a unique tracial state, and has no unbounded densely defined traces [25], Corollary 6.2(i). These simple-algebra hypotheses are not imposed on AA and BB in Theorem 1.1. As a separate regularity consequence, every stabilization A⊗WA\otimes\mathcal{W} in Theorem 1.1 has nuclear dimension at most one, by [26], Theorem 1.3 together with W⊗Z≅W\mathcal{W}\otimes\mathcal{Z}\cong\mathcal{W} from [21], Corollary 6.3. The classification argument below does not use this nuclear-dimension bound.

The traceless case has a different structure: when every extended trace takes only zero and infinity, the trace cone reduces to ideal information. Rørdam’s absorption criterion [29], Theorem 5.2 and Kirchberg’s ideal-lattice classification, with a complete proof in [15], Theorem 6.13, explain the known traceless branch. The present argument must also retain finite trace data and distinguish the regions where a weight is finite from those where it is infinite. That distinction is necessary when finite and infinite subquotients occur in the same algebra.

Restricted nonsimple precedents include Lin and Ng’s classification of certain essential extensions by W\mathcal{W}, with a universal coefficient theorem assumption, a simple quotient, and an invariant containing KK-theory and trace data [24] . The general cone-only question allows arbitrary ideals.

The main analytic tools have separate roles. Ciuperca, Giordano, Ng, and Niu give unital von Neumann algebra uniqueness from support-rank data [7]; we combine this with trace caps and rational averaging to obtain local rank estimates. The stable-uniqueness methods of Dadarlat and Eilers [10] and the ideal-related absorption and multiplier results of Gabe [16], Sections 11–13 remove the resulting errors in norm. Those intermediate results apply here without pure infiniteness of the auxiliary targets. In the existence argument, Connes’s hyperfiniteness theorem [8], nuclear completely positive approximation [6], and measured-field methods [34] provide the classical inputs. The fixed controllers, lower ideal-support estimates, and fine-label correction that connect these tools are proved below.

The strategy of lifting tracial data and then correcting a map through an extension has a methodological precedent in Schafhauser’s proof of the Tikuisis–White–Winter theorem [31]. His setting uses a faithful amenable trace and the universal coefficient theorem (UCT); the present local error ideals and support estimates address a different invariant, with no UCT assumption. The use of quotient cone approximations and carriers in prescribed ideals also has a precedent in Bosa–Gabe–Sims–White [2]. Here the small UHF fractions must satisfy both upper trace bounds and lower comparisons into fixed positive cuts. The suspension-and-corner passage follows the method in [15] and [16]; its trace normalization is proved below for all extended weights.

The construction

Fix

P=A⊗W⊗K,Q=B⊗W⊗K.P = A \otimes\mathcal{W} \otimes\mathcal{K}, \qquad Q = B \otimes\mathcal{W} \otimes\mathcal{K}.

For a C∗C^*-algebra CC, the Cuntz semigroup Cu⁡(C)\operatorname{Cu}(C) consists of Cuntz classes [a][a] of positive elements in C⊗KC \otimes\mathcal{K}, with addition by orthogonal sum. The relation a≾ba \precsim b means that vn∗bvn→av_n^* b v_n \to a in norm for some sequence (vn)(v_n); it determines the order on these classes. Two elements define the same class when each is Cuntz subequivalent to the other. For a positive contraction aa, its rank at an extended trace is dτ(a)=lim⁡kτ(a1/k)d_\tau(a) = \lim_{k} \tau(a^{1/k}), using unnormalized matrix traces. This depends only on [a][a]. Two obstacles distinguish this setting from one with a single normalized trace. A positive element generating a stable algebra may have infinite rank at every nonzero densely finite trace, so making its rank a small scalar multiple gives no useful finite error bound. Also, a weight can be finite only on a proper ideal. We must control errors separately on these ideals and preserve enough lower support to retain the infinite values outside them.

The given cone isomorphism yields compatible isomorphisms

F ⁣:T(Q)⟶T(P),G ⁣:Cu⁡(P)⟶Cu⁡(Q),dτ(G[a])=dFτ(a).F \colon T(Q) \longrightarrow T(P), \qquad G \colon\operatorname{Cu}(P) \longrightarrow\operatorname{Cu}(Q), \qquad d_\tau(G[a]) = d_{F\tau}(a).

We identify the primitive ideal spaces through this correspondence and denote the common space by XX. For an open U⊆XU \subseteq X, write P(U)P(U) and Q(U)Q(U) for the corresponding closed ideals. We first construct maps into a sequence algebra, where errors may tend to zero along the coordinates. Norm uniqueness will later allow their coordinate maps to be conjugated into convergent sequences in QQ. Our intermediate maps take values in

D=Q∞=ℓ∞(Q)/c0(Q).D = Q_\infty= \ell^\infty(Q)/c_0(Q).

We regard QQ as the constant sequences in DD. If ω\omega is a free ultrafilter on N\mathbb{N} and τn∈T(Q)\tau_n \in T(Q), their regularized limit on bounded positive sequences is

ρ([(xn)])=sup⁡ε>0lim⁡n→ωτn((xn−ε)+),xn≥0.\rho([(x_n)]) = \sup_{\varepsilon> 0} \lim_{n \to\omega} \tau_n((x_n - \varepsilon)_+), \qquad x_n \ge0.

Section 3 proves that this defines an extended trace. We use YY equal to a point, a half-open interval, or R\mathbb{R}, with a full-support Radon measure mm, finite on the interval. For ν∈T(P)\nu\in T(P), write Fin⁡(ν)\operatorname{Fin}(\nu) for the closed ideal generated by the positive elements on which ν\nu is finite. The product trace m⊗νm \otimes\nu is the integrated densely finite trace on C0(Y)⊗Fin⁡(ν)C_0(Y) \otimes\operatorname{Fin}(\nu), extended to be infinity on positive elements outside this ideal. On positive elementary tensors it has value (∫f dm)ν(a)(\int f\,dm)\nu(a), with 0⋅∞=00 \cdot\infty= 0. A model is a homomorphism p ⁣:C0(Y)⊗P→Dp \colon C_0(Y) \otimes P \to D satisfying

ρ∘p=m⊗F(ρ∣Q)\rho\circ p = m \otimes F(\rho|_Q)

for every such regularized limit ρ\rho. The quantifier includes nondensely finite weights. An ideal of C0(Y)⊗PC_0(Y) \otimes P has a fine support, an open subset of Y×XY \times X; its projection to XX is the coarse support used to index local estimates.

The main difficulty is to preserve both the finite and the infinite parts of (1.3). Fix a regularized limit ρ\rho, put σ=ρ∣Q\sigma= \rho|_Q, and write Q(V)=Fin⁡(σ)Q(V) = \operatorname{Fin}(\sigma). On C0(Y)⊗P(V)C_0(Y) \otimes P(V), controlled trace moments will identify the pullback of ρ\rho. This alone does not prevent the pullback from becoming finite on a larger ideal. A separate lower ideal comparison rules that out. Once the finite ideal is exactly C0(Y)⊗P(V)C_0(Y) \otimes P(V), both sides of (1.3) are infinite on every positive element outside it. This two-part recovery is the reason for the following constructions.

Local error ideals and stabilizers. For each open U⊆XU \subseteq X, we define an ideal J(U)⊆DJ(U) \subseteq D using uniform bounds on the ranks of positive cuts. The error at each cut is a scalar tending to zero times the rank of a fixed positive controller cc satisfying c≾(b−δ)+c \precsim(b - \delta)_+ for some b∈Q(U)+b \in Q(U)_+ and δ>0\delta> 0. Such errors are invisible to every regularized weight that is densely finite on Q(U)Q(U). We construct small homomorphisms whose values belong to these ideals and dominate any prescribed countable family of smaller errors. Compact containment of open ideals supplies a common controller when different approximation stages are combined. The two versions in Section 4 have different inputs: one takes a small fraction of an existing model; the other builds a small cone homomorphism before any model is available.

Tracial approximation with lower ideal support. Convex separation and von Neumann algebra approximation construct completely positive cone maps with the required first and second trace moments. The construction simultaneously imposes norm tests whose positive averages force lower rank comparisons. The comparison constant is independent of the averaging multiplicities. This lower signal determines the part of the cone on which a weight must remain infinite. Factor representations and their measurable assembly are used only through cut tests controlled by fixed finite-rank constants.

Correction with all ideal labels retained. A small stabilizer places the multiplicative errors in a sigma-unital hereditary target. Module Stinespring dilation and absorption then correct the cone map. The support estimate is imposed on the entire projected ideal of each input. It therefore survives scaling of the cone variable and makes every dilation weakly equivariant for the finer primitive-space labels. Compact corrections can be compressed to finitely many terms of the original diagonal repeat, with an explicit tail estimate. A second small homomorphism then dominates the correction itself. Adding it back retains the lower ideal comparison, so the finite and infinite parts combine to give the full model equation in Section 7.

Uniqueness and passage to actual maps. For two models with the same data, tracial alignment first makes their difference locally small. A stabilizer drawn from a spare model then allows ideal-related stable uniqueness to remove that difference in norm. The spare is supplied by splitting each model into two UHF halves and replacing the halves successively. This argument, in Section 5, assumes that the two models are given; it does not depend on the later existence theorem. Once corrected cone models exist, an exhaustion of the line gives models with Lebesgue data. Translation covariance and a full crossed-product projection give a model for PP itself. A finite positive partition identity computes the trace of this corner, including infinite values. Uniqueness for every pair of subsequences gives eventual conjugacy between any two sufficiently late coordinate maps. We use these conjugacies to make a subsequence Cauchy in norm on each input; its limit is an actual homomorphism P→QP \to Q. Repeating the construction in the other direction gives a map Q→PQ \to P. Their compositions have the identity data, so approximate intertwining proves Theorem 1.1. Figure 1 displays these dependencies. In particular, the uniqueness theorem is conditional on a pair of models; it is available when the existence construction later supplies them.

Principal model-construction dependencies

Figure 1. Principal model-construction dependencies. The existence and uniqueness arguments meet in the passage from sequence models to actual maps. Shared auxiliary inputs are not drawn separately: the trace-cap and barycenter lemmas in Section 5 are used in Section 6; the absorption and hereditary-support lemmas of Section 5 are used in Section 7. Norm uniqueness is a statement about models when they are given; its proof does not assume the cone-existence theorem. The dashed arrow records its further use in actual-map extraction and the final two-sided intertwining.

Organization and conventions

Theorem 2.1 and Proposition 2.2 collect the structural input. The sequence comparisons and local diagonalization are proved in Proposition 3.6 and Lemma 3.10. The stabilizer construction is Theorem 4.1, and norm uniqueness is Theorem 5.1. The two existence stages are Theorems 6.1 and 7.6; the final passage to an isomorphism is Theorem 8.5.

All algebras and Hilbert spaces are complex. A completely positive contractive map is abbreviated c.p.c. Traces on finite matrix amplifications use the unnormalized matrix trace. The universal UHF algebra is denoted by Q\mathcal{Q}, to distinguish it from the target algebra QQ. Rational diagonal averaging uses the normalized UHF trace only in the averaging direction. The notation V∈UV \in U denotes compact containment in the lattice of open subsets of XX, without a Hausdorff assumption.

The invariant, its ideals, and matrix conventions

The trace cone supplies three inputs to the construction: pointwise comparison of Cuntz classes in QQ, a common lattice of ideals for PP and QQ, and positive elements that control finite collections of rank estimates inside those ideals. We establish these inputs before fixing the matrix identifications used in the approximations. All later comparisons are obtained from the coordinate algebra QQ; passage to a sequence algebra will require bounded witnesses.

Ranks and realification

For a∈(C⊗K)+a \in(C \otimes\mathcal{K})_+, extend τ∈T(C)\tau\in T(C) to matrices by the unnormalized matrix trace and put

dτ(a)=lim⁡k→∞τ(a1/k)(0≤a≤1).(2)d_{\tau}(a) = \lim_{k \to\infty} \tau\left(a^{1/k}\right) \qquad(0 \leq a \leq1). \tag*{(2)}

Rescaling an element to be contractive does not change its rank. The resulting function depends only on its Cuntz class. We write dτ(x)d_\tau(x) also for the value at x∈Cu⁡(C)x \in\operatorname{Cu}(C). The basic cut and integration identities are

dτ(a)=sup⁡ε>0dτ((a−ε)+),τ(a)=∫0∥a∥dτ((a−t)+) dt.(3)d_\tau(a)=\sup_{\varepsilon>0}d_\tau((a-\varepsilon)_+),\qquad\tau(a)=\int_0^{\lVert a\rVert}d_\tau((a-t)_+)\,dt. \tag*{(3)}

These identities use extended nonnegative arithmetic and apply to all the weights in (1). We use the following form of the trace and realification theorems. The assertion about the functional cone is [14], Proposition 4.2, Remark 4.3, and Theorem 4.4; compactness is [14], Theorem 3.7. The realification assertions are [28], Proposition 3.1.1 and Theorems 3.2.1 and 5.1.2.

Theorem 2.1 (Trace realification). For every C∗C^*-algebra CC, the trace cone with topology (1) is compact Hausdorff, and it is second countable when CC is separable. If CC is exact, the assignment τ↦dτ\tau\mapsto d_\tau identifies this cone with the topological cone of functionals on Cu⁡(C)\operatorname{Cu}(C).

For every C∗C^*-algebra CC,

Cu⁡(C⊗W)≅Cu⁡(C)R.\operatorname{Cu}(C\otimes\mathcal{W})\cong\operatorname{Cu}(C)_{\mathbb{R}}.

Realification is determined functorially by the topological functional cone. Its realization as functions on that cone has pointwise order, pointwise addition, and multiplication by positive real scalars. It has the same functional cone as Cu⁡(C)\operatorname{Cu}(C).

Consequently the given trace-cone isomorphism induces isomorphisms

F:T(Q)⟶T(P),G:Cu⁡(P)⟶Cu⁡(Q),dτ(Gx)=dFτ(x).(4)F:T(Q)\longrightarrow T(P),\qquad G:\operatorname{Cu}(P)\longrightarrow\operatorname{Cu}(Q),\qquad d_\tau(Gx)=d_{F\tau}(x). \tag*{(4)}

In particular, for x,y∈Cu⁡(Q)x,y\in\operatorname{Cu}(Q),

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