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arXiv:2610.17060v1 [math.KT] 12 Oct 2026

A higher categorical approach to graded bivariant KK-theories for Real C∗C^{*}-algebras

A nupam Datta ††thanks: Universität Göttingen, anupam.datta@mathematik.uni-goettingen.de
Abstract

We present an ∞\infty-categorical refinement of classical K​KKK-theory and EE-theory for graded, GG-equivariant for a locally compact second countable group GG, Real C∗C^{*}-algebras. As a consequence, we obtain a couple of fiber sequences connecting the different KK-theory spectra, and explicitly analyse the induced endomorphisms on K0K_{0}-groups. We also answer precisely some folklore questions in the area. Among other things, we show that graded K​KKK- and EE-categories are not a Dwyer-Kan localization of graded C∗C^{*}-algebras.

1 Introduction

This article is devoted to studying bivariant KK-theories for C∗C^{*}-algebras found in an index theorist’s toolkit using methods from higher category theory. Recent works of Bunke and coauthors ([13], [17], [11]) have refined the classical K​KKK- and EE-categories of C∗C^{*}-algebras to stable ∞\infty-categories, which then enjoy an ∞\infty-categorical version of the classical (11-categorical) universal properties as mentioned in [33] and [20]. This ∞\infty-categorical enhancement is not just for the satisfaction of the modern homotopy theorist, but also helps segregate the homotopical and analytical aspects of the subject.

In [17], Bunke constructs small stable ∞\infty-categories KKsep!,∞KK^{\operatorname{sep}}_{!,\infty} (where !∈{semi−split⁡(se),exact⁡(ex)}!\in\{\operatorname{semi-split(se),exact(ex)}\} denotes the kind of excision we want to have) by universally enforcing certain properties Kasparov’s K​KKK- and Connes-Higson’s EE-theory are known to satisfy, namely, homotopy invariance, compact stability, !!-excision, and Bott periodicity. The same construction can also be done equivariantly in the presence of the action of locally compact second countable group, as mentioned in [16]. That the homotopy category of K​Kse,∞sepKK^{\operatorname{sep}}_{\operatorname{se},\infty} (resp. K​Kex,∞sepKK^{\operatorname{sep}}_{\operatorname{ex},\infty}) is equivalent to Kasparov’s K​KKK- (resp. Connes-Higson’s EE-)categories can be seen by comparing with the classical universal properties, as is worked out in [17, Section 13]. The advantage of defining bivariant KK-categories as a Dwyer-Kan localization is that one can write functors out of the KK!,∞sepKK_{!,\infty}^{\operatorname{sep}}-categories by verifying that a functor defined on separable C∗C^{*}-algebras satisfies certain properties.

However, [13], [17], [11] have been written exclusively with ungraded C∗C^{*}-algebras. In contrast, most of classical bivariant KK-theories have been applied to problems in geometry and topology in their graded avatar. For example, consider the proof of the Baum-Connes conjecture for a-T-menable groups in Higson-Guentner’s article [32], where a myriad of the exotic functorial properties of the graded EE-category were used. Nevertheless, it is the ungraded KK!KK_{!}-theories11 1 we adopt Bunke’s notation and denote by KK!KK_{!} either K​KKK- or EE-theory, even in the classical contexts. whose universal properties are classically known. Given the importance of the graded theory and the effectiveness of realizing KK!KK_{!} as Dwyer-Kan localizations as mentioned earlier, one can ask the same for the graded KK!KK_{!}-category. It turns out that the answer is in the negative, as shown in Section 4.1. The author does not know if this fact was known earlier. However, not all is lost, and higher categorical refinements of graded KK!KK_{!}-categories can still be provided. Following ideas in an unpublished note of Bunke-Duenzinger (see also [15, Section 2.4]), we define an ∞\infty-categorical refinement of graded, GG-equivariant KK!KK_{!}-category as a certain category of comodules over a distinguished cocommutative coalgebra in KKG2!,∞KK^{G_{2}}_{!,\infty}, the G×C2G\times C_{2}-equivariant, ungraded bivariant KK-category. It turns out that this picture captures the formal properties of the classical graded KK!KK_{!}-categories. The details of this higher categorical refinement of graded bivariant KK-categories is one of the cornerstones of this article, and is developed in Section 4.

The other aspect missing from the writings of Bunke on higher categorical approaches to KK!KK_{!}-theories is a discussion of Real C∗C^{*}-algebras. Apart from being of independent interest, Real K⁡(K)K(K)-theory encodes finer information than its complex counterpart, as for example is clear from the seminal works of Hitchin ([36]) and Rosenberg ([51]). Luckily, the construction of Real KK!,∞KK_{!,\infty}-categories for separable C∗C^{*}-algebras follow the same path as in [17] (see also [11, Section 3.4]), with only one difference: we would have to enforce the well known (1,1)(1,1)-periodicity at the final step of the construction. The construction of stable ∞\infty-categories refining classical Real KK!KK_{!}-categories is the content of the first few subsections of Section 3.22 2 In our treatment of graded KK!KK_{!}-categories, we have worked with Real C∗C^{*}-algebras equipped with the action of an external locally compact group. We did not mention this in the last paragraph because the passage from ungraded to graded is much more drastic than the one from complex to Real. And equivariant matters were already considered in works of Bunke. Unless otherwise mentioned, in this article we work with Real C∗C^{*}-algebras by default.

We now mention some applications of the abstract theory developed in Sections 3 and 4 of this article. In order to streamline the presentation, we package all of them in the next theorem. To simplify the exposition, we also ignore the external (compact) group action here. The (more or less straightforward) generalization to the equivariant case is present in Section 5.

Theorem 1.1.

Denote by 𝕂⁡(−),𝕂C2​(−),𝕂^​(−)\mathbb{K}(-),\mathbb{K}^{C_{2}}(-),\hat{\mathbb{K}}(-) the ungraded (classical), C2C_{2}-equivariant, and graded spectrum valued KK-theory functors on the corresponding categories of (Real) C∗C^{*}-algebras. Let AA be a C∗C^{*}-algebra with a C2C_{2}-action αA\alpha_{A}. Then we have the following33 3 the labels 𝟏,𝟐,𝟑,𝟒\mathbf{1},\mathbf{2},\mathbf{3},\mathbf{4} are just notation and should not be confused with the multiplication with some constant maps!.

  1. 1.

    There is a natural fiber sequence of spectra

    𝕂⁡(Au)→𝟏𝕂C2​(A)→𝟐𝕂^​(A)\mathbb{K}(A_{u})\xrightarrow{\mathbf{1}}\mathbb{K}^{C_{2}}(A)\xrightarrow{\mathbf{2}}\hat{\mathbb{K}}(A)

    Here (−)u(-)_{u} denotes the underlying C∗C^{*}-algebra functor. Furthermore, the fiber sequence splits if AA is inner graded.

  2. 2.

    There is a natural fiber sequence of spectra

    𝕂^​(A)→𝟑𝕂C2​(A)→𝟒𝕂⁡((A​⊗^​C​l0,2)u)\hat{\mathbb{K}}(A)\xrightarrow{\mathbf{3}}\mathbb{K}^{C_{2}}(A)\xrightarrow{\mathbf{4}}\mathbb{K}((A\hat{\otimes}Cl^{0,2})_{u})

    Here A​⊗^​C​l0,2A\hat{\otimes}Cl^{0,2} denotes the graded tensor product of AA and C​l0,2Cl^{0,2}, the Clifford algebra on two generators which square to +1+1. If AA is inner graded, the fiber sequence splits.

  3. 3.

    There are endomorphisms of the different KK-theory spectra of AA arising from the above two fiber sequences. At the level of π0\pi_{0}, their effect can be concretely described when the algebra AA is unital:

    1. (a)

      𝟑∘𝟐∈End⁡(K0C2)​(A)\mathbf{3}\circ\mathbf{2}\in\operatorname{End}(K_{0}^{C_{2}})(A) is given by mapping the class of a C2C_{2}-equivariant projective AA-module [M,αM]∈K0C2​(A)[M,\alpha_{M}]\in K_{0}^{C_{2}}(A) to [M,αM]−[M,−αM][M,\alpha_{M}]-[M,-\alpha_{M}].

    2. (b)

      𝟐∘𝟑∈End⁡(K^0​(A))\mathbf{2}\circ\mathbf{3}\in\operatorname{End}(\hat{K}_{0}(A)) is given by mapping the class of a Fredholm cycle44 4 see Section 2.2. (ℰ,F)∈K0Fr​(A)(\mathcal{E},F)\in K_{0}^{\operatorname{Fr}}(A) to (ℰ⊕ℰ,F⊕−F)∈K0Fr​(A)(\mathcal{E}\oplus\mathcal{E},F\oplus-F)\in K_{0}^{\operatorname{Fr}}(A).

    3. (c)

      When AA is inner graded or AA is complex, then 𝕂⁡((A​⊗^​C​l0,2)u)≃𝕂⁡(Au)\mathbb{K}((A\hat{\otimes}Cl^{0,2})_{u})\simeq\mathbb{K}(A_{u}), and the map 𝟒∘𝟏∈End⁡(K0​(Au))\mathbf{4}\circ\mathbf{1}\in\operatorname{End}(K_{0}(A_{u})) is given by mapping the class of a finitely generated projective AA-module [M]∈K0​(A)[M]\in K_{0}(A) to [M⊕Mα]∈K0​(A)[M\oplus M_{\alpha}]\in K_{0}(A), where MαM_{\alpha} has the same underlying abelian group M¯\underline{M} as MM, and the AA-action is given by m¯.a:=m​αA​(a)¯.\underline{m}.a:=\underline{m\alpha_{A}(a)}.

    4. (d)

      Under the same assumption on AA as in the last point, the map 𝟏∘𝟒∈End⁡(K0C2​(A))\mathbf{1}\circ\mathbf{4}\in\operatorname{End}(K_{0}^{C_{2}}(A)) is given by mapping the class of a C2C_{2}-equivariant finitely generated projective AA-module [M,αM]∈K0C2​(A)[M,\alpha_{M}]\in K_{0}^{C_{2}}(A) to [M⊕M,(m,n)↦(αM(n),αM(m))]∈K0C2(A)[M\oplus M,(m,n)\mapsto(\alpha_{M}(n),\alpha_{M}(m))]\in K_{0}^{C_{2}}(A).

Before describing the organization of this article, we mention the relation between our fiber sequences and the Clifford module quotient55 5 the author learnt this sleek term from a talk of Luuk Stehouwer at the Max Planck Institute for Mathematics in 2025. picture of KK-theory of a point as described by Atiyah, Bott and Shapiro in [4]. Roughly speaking, one of the main results of loc.​ cit.​ (see also [41, Section I.9]) is the following (recall that C​lp,qCl^{p,q} denotes the Clifford algebra on p+qp+q generators, where pp generators square to −1-1, and qq generators square to +1+1.)

Theorem 1.2.

(Atiyah-Bott-Shapiro) For every non-negative integer nn, there is a canonical isomorphism of abelian groups

K−n​(∗)≅{finitely​generated​graded​Cln,0−modules}gp{finitely​generated​graded​Cln+1,0−modules}gpK^{-n}(*)\cong\frac{\{\operatorname{finitely\penalty\ generated\penalty\ graded\penalty\ Cl^{n,0}-modules}\}^{\operatorname{gp}}}{\{\operatorname{finitely\penalty\ generated\penalty\ graded\penalty\ Cl^{n+1,0}-modules}\}^{\operatorname{gp}}}

It can be seen (Section 5.1) that Theorem 1.2 is asserting that the long exact sequence of homotopy groups of the fiber sequence labeled “ABS” splits off into short exact sequences when AA is a Clifford algebra. Our results therefore clarifies the situation for a general graded, Real (GG-equivariant for a compact group GG) C∗C^{*}-algebra: replace the process of taking cokernels in abelian groups by taking cofiber in spectra. This also answers a folklore question pertaining to whether higher KK-groups of a C∗C^{*}-algebra can be given a Clifford module quotient description analogous to Theorem 1.2; see Section 5.1 for details.

As the reader may guess, the other fiber sequence labeled “van Daele” has been tagged so because it recovers the classical definition of van Daele KK-theory ([60],[61]). After a bit of massaging66 6 by working with the (graded) opposite C∗C^{*}-algebra, this sequence can be seen to recover Karoubi’s definition of graded KK-theory ([38, Chapitre II.2.1]) as well. We do not delve into these comparisons (and the inter-comparisons) in this article, and point the curious reader to the work of David Aretz and Luuk Stehouwer ([3]), where such considerations have been discussed in detail. Note that loc.​ cit.​ is written in the generality of Banach algebras, and our fiber sequence “ABS” is more or less their definition of the graded KK-theory spectrum (see [3, Definitions 3.42 & 3.55]).

Finally, we mention that Ulrich Haag has works ([30],[31]) in this area. Therein, Haag obtains a couple of long exact sequences involving the different flavors of KK-groups, but only for complex C∗C^{*}-algebras. It can be seen that exactly one of Haag’s sequences survives the Real case, and the other one does not. The sequence that survives can be readily identified with the long exact sequence of homotopy groups of our sequence “ABS”. In the author’s view, some of the proofs presented in his papers would benefit from a more detailed and transparent exposition. Hence the methods of higher categories used in this paper both generalize and clarify Haag’s works.

1.1 Organization of the article

We now discuss the organization of this article.

Section 2 contains well-known results from equivariant and graded KK-theory. The key highlights of this section are Theorem 2.3 and Section 2.2. The non-equivariant case of Theorem 2.3 is the content of [26], and the equivariant generalization is more or less straightforward. Section 2.2 contains some miscellaneous results on the graded KK-theory of a distinguished graded C∗C^{*}-algebra 𝒮\mathcal{S}, and the results therein are going to be really crucial in the later sections.

In Section 3, we emulate the analogous chapters of [17], and construct a stable ∞\infty-categorical refinement of the GG-equivariant, Real K​KKK- and EE-categories. We actually combine the approaches of [17] and [11]; Section 3.3 is taken from the relevant section of [11]. In Section 3.4, we (have to) deviate from the writings of Bunke and work with a Real variant of the Toeplitz extension so as to enforce (1,1)(1,1)-periodicity. The category so obtained is denoted by KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}, where !∈{se,ex}!\in\{\operatorname{se,ex}\} denotes whether we enforced excision for semi-split exact or all exact sequences. Section 3.5 discusses the well-known change of group functors: restriction, induction and coinduction. These come in handy while studying the graded theory, although in the simple case with the groups involved being GG and G2:=G×C2G_{2}:=G\times C_{2}. Section 3.6 makes connections with the models of equivariant and graded KK-theory as studied in Section 2 with certain corepresentable functors out of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} (see Theorem 3.14 for a precise statement). Finally in Section 3.7, the extension of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} to the large category of all GG-C∗C^{*}-algebras is considered.

Section 4 contains the higher categorical approach to defining the graded bivariant KK-categories, which we denote by KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}. Without apriori knowing that the homotopy category of KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} recovers classical graded K​KKK- and EE-theory according as !=se!=\operatorname{se} or !=ex!=\operatorname{ex}, we show that the formal consequences of our definition, together with a calculation in classical graded KK-theory yields the familiar equivalence between C0​(ℝ0,1)C_{0}(\mathbb{R}^{0,1}) and C​l1,0Cl^{1,0} in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}. We also connect the spectral model of KK-theory as discussed in Section 2 with the functor corepresented by ℂ\mathbb{C} in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}.

Section 5 is devoted to deducing Theorem 1.1 as a consequence of the machinery developed in Sections 3 and 4. As advertised before, in this section we also discuss the folklore question of representing graded KK-groups of a (graded), (Real) unital C∗C^{*}-algebra in terms of Clifford module quotients.

Finally in Section 6, we compare the homotopy categories of the ungraded and graded KKG!,∞KK^{G}_{!,\infty}-categories we developed with the classical ungraded and graded K​KGKK^{G}- and EGE^{G}-categories (upon restricting to separable C∗C^{*}-algebras; the general comparison is discussed in Section 6.1). We give more details in the context of EE-theory: the well-known universal property of ungraded EE-theory lacks a proof in the foundational writings [20] and [29], and a detailed proof (following the work of Thomsen in [59]) is provided in Section 6.2. In Section 6.3, we discuss an equivariant generalization of a technical result of Dadarlat and Loring, which is an intermediary in making the comparison of the homotopy category of KK^ex,∞G,sep\widehat{\mathrm{KK}}_{\mathrm{ex},\infty}^{G,\mathrm{sep}} (denoted KK^ex,0G,sep\widehat{\mathrm{KK}}_{\mathrm{ex},0}^{G,\mathrm{sep}}) and E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}}. We mention that the comparison of the homotopy category of KK^se,∞G,sep\widehat{\mathrm{KK}}_{\mathrm{se},\infty}^{G,\mathrm{sep}} (denoted KK^se,0G,sep\widehat{\mathrm{KK}}_{\mathrm{se},0}^{G,\mathrm{sep}}) and KK^KasG,sep\widehat{\mathrm{KK}}_{\mathrm{Kas}}^{G,\mathrm{sep}} is not directly possible using the techniques we used for their EE-theoretic counterparts, but instead can be deduced from results of Meyer ([46]).

Acknowledgments: The author is deeply grateful to Johannes Ebert for suggesting this project, his generous guidance throughout, and his thoughtful comments on earlier drafts. Many thanks to David Aretz and Luuk Stehouwer for having several pleasant discussions on topics related to this article, and also for freely sharing some ideas from their recent (and related) project. The author would also like to thank Ulrich Bunke, Benjamin Duenzinger, Michael Joachim, Matthias Lesch, Yuezhao Li and Maxime Ramzi for discussions at several points which clarified some mathematical issues.

This paper forms part of the PhD thesis of the author at the University of Bonn. Throughout the duration of his PhD, the author was supported by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany’s Excellence Strategy – GZ 2047/1 - 390685813, Hausdorff Center for Mathematics.

2 Background on KK-theory spaces, groups, and some calculations

In this section, we discuss the necessary background from classical / equivariant / graded KK-theory that will be needed in the later sections. We emphasize that (morally) KK-theory is a significantly simpler concept than K​KKK-theory, and we use our knowledge of KK-theory as discussed in this section later while studying the bivariant KK-categories.

Before proceeding further, we have to introduce the main objects of the entire project, namely, graded, Real, equivariant C∗C^{*}-algebras.

Definition 2.0.
  1. 1.

    A graded complex C∗C^{*}-algebra (A,ε)(A,\varepsilon) is a complex C∗C^{*}-algebra AA equipped with a ∗*-automorphism ε\varepsilon such that ε2=1\varepsilon^{2}=1. ε\varepsilon is called the grading on AA. The elements of the +1+1 and −1-1 eigenspaces of AA are called even and odd, respectively.

  2. 2.

    For GG a locally compact second countable group, a complex GG-C∗C^{*}-algebra (A,α)(A,\alpha) is a C∗C^{*}-algebra AA together with a continuous homomorphism α:G→Aut⁡(A)\alpha:G\rightarrow\operatorname{Aut}(A), where Aut⁡(A)\operatorname{Aut(A)} is equipped with the point-norm topology.

  3. 3.

    A Real C∗C^{*}-algebra (A,τ)(A,\tau) is a complex C∗C^{*}-algebra AA equipped with a ℂ\mathbb{C}-anti-linear ∗*-automorphism τ\tau such that τ2=1\tau^{2}=1. τ\tau is called the Real structure on AA. 77 7 Sometimes, the Real structure will simply be denoted by a↦a¯a\mapsto\bar{a}. The real C∗C^{*}-algebra associated to (A,τ)(A,\tau) is Aτ:={a∈A∣a=τ⁡(a)}A_{\tau}:=\{a\in A\mid a=\tau(a)\}, and it can be shown that this induces an equivalence of categories between real and Real C∗C^{*}-algebras.

  4. 4.

    For any two (or all three) of the adjectives defined before, we combine them in the obvious way by requiring the corresponding structure maps to commute.

Notation 2.0.

We follow the following conventions throughout this article.

  • •

    Unless otherwise mentioned, GG will denote a locally compact second countable group.

  • •

    As already mentioned in the introduction, we will by default be working be working with Real C∗C^{*}-algebras. Results in the complex case can be deduced by simply ignoring the Real structure. We do not mention the word “Real” unless there is an explicit need to do so.

  • •

    We denote the category of (ungraded) Real GG-C∗C^{*}-algebras (with the obvious morphisms) by 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}. This category is enriched over topological spaces using the point-norm topology on the hom sets (see [26, Section 2.2] for details), and the mapping space is denoted by Hom¯G​(A,B)\underline{\operatorname{Hom}}_{G}(A,B). The set of path componentns of Hom¯G​(A,B)\underline{\operatorname{Hom}}_{G}(A,B) is denoted by [A,B]G[A,B]_{G}. If it is clear from the context, we suppress the GG from the notation.

  • •

    The symmetric monoidal structures on 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg} will be denoted by −⊗?−-\otimes_{?}-, where ?∈{min,max}?\in\{\min,\max\} corresponds to the minimal and maximal tensor products. If an algebra under consideration is nuclear, we often omit the decoration from the tensor product.

  • •

    We denote the category of graded, Real GG-C∗C^{*}-algebras (with the obvious morphisms) by 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}. Its symmetric monoidal structures will be denoted by −⊗^?−-\hat{\otimes}_{?}-, where ?∈{min,max}?\in\{\min,\max\} corresponds to the graded minimal and maximal tensor products. If an algebra under consideration is nuclear, we often omit the decoration from the tensor product (see also [63, Corollary E.2.19]). 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg} is also topologically enriched in a way analogous to the ungraded case mentioned above; the only difference being that the desired equivariance now is with respect to G×C2G\times C_{2}.

  • •

    Finally, we remark that in exceptional cases where we do have to work with the category of complex C∗C^{*}-algebras (for example, in Section 5.2), we keep using the same notation as above. This should not create any confusion.

We next mention some examples of graded C∗C^{*}-algebras which we will often encounter. Further examples and discussions can be found in [26]

Example 2.0.
  1. 1.

    The base field ℂ\mathbb{C} is trivially graded, and is always equipped with the trivial GG-action. In the Real situation, the Real structure on ℂ\mathbb{C} is given by pointwise complex conjugation, and is omitted from the notation.

  2. 2.

    The Clifford algebras come with a natural grading, and carry the trivial action of the external group GG.

  3. 3.

    𝒮:=C0​(ℝ)\mathcal{S}:=C_{0}(\mathbb{R}) with the even-odd grading, trivial GG-action, and the Real structure given by pointwise complex conjugation is going to be a very important algebra for us. By choosing an odd, increasing homeomorphism between (−1,1)(-1,1) and ℝ\mathbb{R} (the choice of this homeomorphism does not matter as the space of all such homeomorphisms is contractible), we obtain an isomorphism between 𝒮\mathcal{S} and 𝒮~\tilde{\mathcal{S}}, the bounded transform of 𝒮\mathcal{S}. We mention another perspective on 𝒮~\tilde{\mathcal{S}} below, which comes very handy in concrete situations. Consider the map

    Φ:𝒮~\displaystyle\Phi:\tilde{\mathcal{S}} →{f:[0,1)→Cl0,1∣f(0)∈ℂ⊆Cl0,1}⊆C0([0,1),Cl0,1)\displaystyle\rightarrow\{f:[0,1)\rightarrow Cl^{0,1}\mid f(0)\in\mathbb{C}\subseteq Cl^{0,1}\}\subseteq C_{0}([0,1),Cl^{0,1})
    f\displaystyle f ↦fev∣[0,1)+ε​fodd∣[0,1),\displaystyle\mapsto f_{\operatorname{ev}}\mid_{[0,1)}+\varepsilon f_{\operatorname{odd}}\mid_{[0,1)},

    where fev,foddf_{\operatorname{ev}},f_{\operatorname{odd}} denote the even and odd parts of ff respectively, and ε\varepsilon is the non-trivial generator of C​l0,1Cl^{0,1}. Φ\Phi can directly be checked to be an isomorphism in 𝖢^∗​𝖠𝗅𝗀\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}.

  4. 4.

    A grading on a C∗C^{*}-algebra is said to be inner if it is given by conjugation with a self-adjoint unitary in the multiplier algebra of AA. If AA is furthermore equivariant and/or Real, the unitary needs to satisfy the required invariance conditions. The algebras of GG-continuous bounded and compact operators on a graded GG-Hilbert space are naturally inner graded. The Clifford algebra C​lp,qCl^{p,q} is inner graded if p−q≡0​(mod⁡4)p-q\equiv 0\penalty\ (\operatorname{mod}4).

Before proceeding, we set up some shorthand notation that we will be using throughout this article.

Notation 2.0.

We denote by G2G_{2} the group G×C2G\times C_{2} (equipped with the product topology).

Remark 2.0.

Although the categories 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg} and 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg} are equivalent (by definition!), the symmetric monoidal structures on them are different. See [3, Section 3.1] for a categorical perspective on the symmetric monoidal structures on 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}.

We now begin our study of KK-theory. As is customary in the development of equivariant KK-theory, we obtain interesting results when the action is by a compact group. So throughout the remainder of this section, GG will denote a compact group.

2.1 Miscellaneous results on equivariant (ungraded) KK-theory

In this subsection, we record some well known results in the realm of equivariant KK-theory following [8, Chapter 11]. Recall that (by definition) the equivariant K0K_{0}-group of a unital GG-C∗C^{*}-algebra is the Grothendieck group of the abelian monoid (under direct sum) of finitely generated, GG-equivariant projective AA-modules. We summarize some well-known properties of the equivariant KnK_{n}-functors in the next remark for the ease of reference later.

Remark 2.0.

The following facts about GG-equivariant KK-theory are well-known.

  1. 1.

    K0G​(ℂ)K_{0}^{G}(\mathbb{C}) is a ring with multiplication obtained from the external tensor product of GG-vector spaces, and is isomorphic to R⁡(G)R(G), the representation ring of GG. In particular, the ring K0C2​(ℂ)K_{0}^{C_{2}}(\mathbb{C}) is isomorphic to ℤ⁡[x]x2=1\frac{\mathbb{Z}[x]}{x^{2}=1}, the group ring of C2C_{2}. The preferred isomorphism maps the trivial representation of C2C_{2} on ℂ\mathbb{C} to 1∈ℤ⁡[x]x2=11\in\frac{\mathbb{Z}[x]}{x^{2}=1} and the sign representation of C2C_{2} on ℂ\mathbb{C} to x∈ℤ⁡[x]x2=1x\in\frac{\mathbb{Z}[x]}{x^{2}=1}.

  2. 2.

    More generally, the external product with an element of K0G​(ℂ)K^{G}_{0}(\mathbb{C}) refines KnG​(−)K^{G}_{n}(-) to functors 88 8 this should not be confused with the “GG-action on KGK^{G}-groups induced by the action on the algebra”, because in general there is no such action! When GG is C2C_{2}, then this action exists, but can be shown to be always trivial.

    KnG​(−):𝖦𝖢∗​𝖠𝗅𝗀→R⁡(G)​-​Mod​∀n≥0K_{n}^{G}(-):\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow R(G)\text{-}\operatorname{Mod}\forall\penalty\ n\geq 0
  3. 3.

    Of importance to us is the Green-Julg theorem, which asserts that there is a natural isomorphism

    KnG​(A)≅Kn​(A⋊G)​∀n≥0K^{G}_{n}(A)\cong K_{n}(A\rtimes G)\penalty\ \forall\penalty\ n\geq 0

    See [8, Theorem 11.7.1] for a proof. For the case of G=C2G=C_{2}, note that we have a natural isomorphism A⋊C2≅(A​⊗^​C​l0,1)uA\rtimes C_{2}\cong(A\hat{\otimes}Cl^{0,1})_{u} (see [8, Proposition 14.5.1]) and will sometimes use this identification without mentioning.

For our applications later, we need to compute the C2C_{2}-equivariant KK-groups of the graded C∗C^{*}-algebras C​l0,1Cl^{0,1} and 𝒮\mathcal{S}. Though the calculations of these groups are surely well known, we include in the proofs some details which will come handy in Section 5.

Proposition 2.0.

KnC2​(C​l0,1)≅Kn​(ℂ)​∀n∈ℕ≥0K_{n}^{C_{2}}(Cl^{0,1})\cong K_{n}(\mathbb{C})\penalty\ \forall\penalty\ n\in\mathbb{N}_{\geq 0}. The C2C_{2}-action on KnC2​(C​l0,1)K_{n}^{C_{2}}(Cl^{0,1}) induced by K0C2​(ℂ)K_{0}^{C_{2}}(\mathbb{C}) (as dictated by Section 2.1.2) is given by the identity.

Proof.

We begin by analyzing the maps

KnC2​(ℂ)→ι∗KnC2​(C​l0,1).K_{n}^{C_{2}}(\mathbb{C})\xrightarrow{\iota_{*}}K_{n}^{C_{2}}(Cl^{0,1}).

Consider the commutative diagram (with the unlabeled horizontal arrow us so defined to render the diagram commutative)

KnC2​(ℂ){\lx@inpgf@ignorespaces{K_{n}^{C_{2}}(\mathbb{C})}}KnC2​(C​l0,1){\lx@inpgf@ignorespaces{K_{n}^{C_{2}}(Cl^{0,1})}}Kn​(C​lu0,1){\lx@inpgf@ignorespaces{K_{n}(Cl^{0,1}_{u})}}Kn​(C​lu0,2)≅Kn​(M2​(ℂu)){\lx@inpgf@ignorespaces{K_{n}(Cl^{0,2}_{u})\cong K_{n}(M_{2}(\mathbb{C}_{u}))}}Kn​(ℂ)⊕Kn​(ℂ){\lx@inpgf@ignorespaces{K_{n}(\mathbb{C})\oplus K_{n}(\mathbb{C})}}Kn​(ℂ){\lx@inpgf@ignorespaces{K_{n}(\mathbb{C})}}ι∗\scriptstyle{\lx@inpgf@ignorespaces\iota_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}(ι​⊗^​C​l0,1)u\scriptstyle{\lx@inpgf@ignorespaces(\iota\hat{\otimes}Cl^{0,1})_{u}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}

where the top vertical isomorphisms are induced by the Green-Julg theorem, and the lower vertical isomorphisms are induced by the canonical maps. We claim that the bottom horizontal map is given by addition. To that end, one checks that the inclusion C​l0,1→C​l0,2Cl^{0,1}\rightarrow Cl^{0,2} corresponds to the homomorphism

ℂ⊕ℂ\displaystyle\mathbb{C}\oplus\mathbb{C} →M2​(ℂ)\displaystyle\rightarrow M_{2}(\mathbb{C})
(x,y)\displaystyle(x,y) ↦12​(x+yx−yx−yx+y).\displaystyle\mapsto\frac{1}{2}\begin{pmatrix}x+y&x-y\\ x-y&x+y\end{pmatrix}.

under the standard identifications. Precomposing with the two inclusions of ℂ\mathbb{C} into (ℂ⊕ℂ)u(\mathbb{C}\oplus\mathbb{C})_{u} therefore induce the homomorphisms ℂ→M2​(ℂ)u\mathbb{C}\rightarrow M_{2}(\mathbb{C})_{u} given by

λ↦12​(λλλλ)andμ↦12​(μ−μ−μμ).\lambda\mapsto\frac{1}{2}\begin{pmatrix}\lambda&\lambda\\ \lambda&\lambda\end{pmatrix}\penalty\ \penalty\ \text{and}\penalty\ \penalty\ \mu\mapsto\frac{1}{2}\begin{pmatrix}\mu&-\mu\\ -\mu&\mu\end{pmatrix}.

The two homomorphisms can be homotoped to the left-upper-corner inclusion and/or the right-lower-corner inclusion. The claim now follows from [63, Lemma 2.7.6].

To understand the C2C_{2}-action on KnC2​(C​l0,1)K_{n}^{C_{2}}(Cl^{0,1}) induced by K0C2​(ℂ)K_{0}^{C_{2}}(\mathbb{C}), one notes that the flip action on K0C2​(ℂ)K_{0}^{C_{2}}(\mathbb{C}) is invariant under the addition map, and that ι∗\iota_{*} is an ℤ⁡[C2]\mathbb{Z}[C_{2}]-module homomorphism. ∎

Corollary 2.0.

K0C2​(𝒮)≅ℤK_{0}^{C_{2}}(\mathcal{S})\cong\mathbb{Z}. The C2C_{2}-action on K0C2​(𝒮)K_{0}^{C_{2}}(\mathcal{S}) induced by K0C2​(ℂ)K_{0}^{C_{2}}(\mathbb{C}) is given by n↦−nn\mapsto-n.

Proof.
99 9 We probably are not giving the cleanest of this result! Instead, we mention in the proof some ideas which we will use later. We are also implicitly identifying 𝒮\mathcal{S} with the bounded transform 𝒮~\tilde{\mathcal{S}} of 𝒮\mathcal{S} in this proof.

Consider the diagram in 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}

ker⁡(ev1){\lx@inpgf@ignorespaces{\ker(\operatorname{ev}_{1})}}{f:[0,1]→Cl0,1∣f(0)∈ℂ⊆Cl0,1}{\lx@inpgf@ignorespaces{\{f:[0,1]\rightarrow Cl^{0,1}\mid f(0)\in\mathbb{C}\subseteq Cl^{0,1}\}}}C⁡([0,1],C​l0,1){\lx@inpgf@ignorespaces{C([0,1],Cl^{0,1})}}𝒮~{\lx@inpgf@ignorespaces{\tilde{\mathcal{S}}}}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}C​l0,1{\lx@inpgf@ignorespaces{Cl^{0,1}}}Φ,≅\scriptstyle{\lx@inpgf@ignorespaces\Phi,\cong}ev0,≃\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev_{0}},\simeq}ev1\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{1}}ev0,≃\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev_{0}},\simeq}ev0\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev_{0}}}ι\scriptstyle{\lx@inpgf@ignorespaces\iota} (2.1)

where Φ\Phi is as in Section 2.3. Note that the right square is a pullback square (it is the defining square of the mapping cylinder construction; see also Section 3.1.2), and the left square as well as the two triangles involving the dashed edge commute up to homotopy. The rest follows by applying the K0C2​(−)K_{0}^{C_{2}}(-) functor to Equation 2.1, using the homotopy invariance and exicision properties of equivariant KK-theory and the proof of Section 2.1. Observe that the kernel of the addition map ℤ⊕ℤ→ℤ\mathbb{Z}\oplus\mathbb{Z}\rightarrow\mathbb{Z} is {(n,−n)∣n∈ℤ},\{(n,-n)\mid n\in\mathbb{Z}\}, which is evidently isomorphic to ℤ\mathbb{Z} with the action n↦−nn\mapsto-n. ∎

We now want to present a generator of K0C2​(𝒮)≅ℤK_{0}^{C_{2}}(\mathcal{S})\cong\mathbb{Z}. To that end, we need a concrete model for the C2C_{2}-equivariant K0K_{0}-group of a non-unital C∗C^{*}-algebra. This picture is going to be convenient for later use, especially in Section 3.6.

We begin with the relevant definitions.

Definition 2.1.

Let AA be a separable GG-C∗C^{*}-algebra. Set Q​A:=A∗AQA:=A*A, the coproduct in the category of separable GG-C∗C^{*}-algebras. Denote by q​AqA the kernel of the fold map Q​A→AQA\rightarrow A. q​AqA gets a natural GG-action from AA.

Remark 2.1.

The following remarks about q​AqA are in order.

  1. 1.

    q​AqA fits in a short exact sequence

    0→q​A→Q​A→A→0.0\rightarrow qA\rightarrow QA\rightarrow A\rightarrow 0.

    The sequence splits in two canonical ways, depending on embedding AA into one of the components of Q​AQA.

  2. 2.

    The qq construction is functorial, and there are two natural maps q​A→AqA\rightarrow A given by restricting the homomorphisms

    A∗A→(1A,0)A,A∗A→(0,1A)AA*A\xrightarrow{(1_{A},0)}A,\penalty\ \penalty\ \penalty\ \penalty\ A*A\xrightarrow{(0,1_{A})}A

    to q​AqA.

  3. 3.

    Given A,B∈𝖦𝖢∗​𝖠𝗅𝗀A,B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}, a prequasi-homomorphism from AA to BB consists of a GG-C∗C^{*}-algebra EE, two GG-equivariant ∗*-homomorphisms1010 10 α¯\overline{\alpha} should not be confused with any sort of complex conjugation! α,α¯:A→E\alpha,\overline{\alpha}:A\rightarrow E, an ideal J⊲EJ\triangleleft E, and a GG-equivariant ∗*-homomorphism μ:J→B\mu:J\rightarrow B such that α⁡(x)−α¯​(x)∈J​∀x∈A\alpha(x)-\overline{\alpha}(x)\in J\penalty\ \forall\penalty\ x\in A. We write it as

    A{\lx@inpgf@ignorespaces{A}}E⊳J{\lx@inpgf@ignorespaces{E\triangleright J}}B{\lx@inpgf@ignorespaces B}α¯\scriptstyle{\lx@inpgf@ignorespaces\overline{\alpha}}α\scriptstyle{\lx@inpgf@ignorespaces\alpha}μ\scriptstyle{\lx@inpgf@ignorespaces\mu}

    By universal properties, a prequasi-homomorphism A→BA\rightarrow B yields a map μ∘q⁡(α,α¯):q​A→B\mu\circ q(\alpha,\overline{\alpha}):qA\rightarrow B, which we simply denote by α−α¯\alpha-\overline{\alpha}.

  4. 4.

    When A=ℂA=\mathbb{C}, there is a concrete description of q​ℂq\mathbb{C}:

    q​ℂ≅{f∈C0​((0,1],M2​(ℂ))∣f⁡(1)​is diagonal}.q\mathbb{C}\cong\{f\in C_{0}((0,1],M_{2}(\mathbb{C}))\mid f(1)\penalty\ \text{is diagonal}\}.

    This is stated in [8, Exercise 10.11.13.g], and a proof with a lot of details and other background is available in [54]. Technically, loc.​ cit.​ gives a concrete function algebra description of the universal unital C∗C^{*}-algebra on two projections, from which our result can be directly deduced in light of the defining short exact sequence of q​ℂq\mathbb{C} as mentioned in the first remark above. See also [21, Section 6].

  5. 5.

    The above isomorphism directly shows that, in light of Section 2.3,

    𝒮⋊C2≅(𝒮​⊗^​C​l0,1)u≅q​ℂ.\mathcal{S}\rtimes C_{2}\cong(\mathcal{S}\hat{\otimes}Cl^{0,1})_{u}\cong q\mathbb{C}.

    This bridges the gap between the spectral model (studied in the next subsection) and the Cuntz picture. In particular, the proof of the next proposition can also be deduced from Theorem 2.3 in light of a restriction-coinduction adjunction at the level of the compact-stabilized homotopy categories. Similar ideas are used in the proof of Section 3.6.

  6. 6.

    An important technical feature of q​ℂq\mathbb{C} is semi-projectivity, which implies that for all A∈𝖦𝖢∗​𝖠𝗅𝗀A\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}, the canonical map

    [q​ℂ,A]G→≅[[q​ℂ,A]]G[q\mathbb{C},A]_{G}\xrightarrow{\cong}[[q\mathbb{C},A]]_{G}

    from the GG-equivariant homotopy classes of maps to the GG-equivariant asymptotic homotopy classes of maps from q​ℂq\mathbb{C} to AA is a bijection of sets. See [8, Exercise 4.7.1, Proposition 25.1.7] and [Blackadar1985Shape] for general results on semi-projective C∗C^{*}-algebras. The proof of q​ℂq\mathbb{C} being semi-projective is the content of [42, Theorem 7].

Proposition 2.1.

Let GG be a compact group and AA a GG-C∗C^{*}-algebra. Then, there is a natural isomorphism of abelian groups

[q​ℂ,A⊗𝒦⁡(L2​Gℕ)]G≅K0G​(A).[q\mathbb{C},A\otimes\mathcal{K}(L^{2}G_{\mathbb{N}})]_{G}\cong K_{0}^{G}(A).
Proof.

The result is well known, see for example [8, Section 17.6], [22, Remark 1]. The compact group action (and the Real structure) do not cause any extra difficulty as GG-equivariant1111 11 GG-equivariant adjointable operators are precisely the GG-fixed points of the GG-C∗C^{*}-algebra of adjointable operators on a GG-Hilbert module., GG-continuous Fredholm operators on GG-Hilbert modules classify GG-equivariant K0K_{0} when GG is compact; see Theorem 2.3.5 for example. ∎

Remark 2.1.

We mention that the isomorphism

K0G​(A)\displaystyle K_{0}^{G}(A) →≅[q​ℂ,A⊗𝒦⁡(L2​Gℕ)]G\displaystyle\xrightarrow{\cong}[q\mathbb{C},A\otimes\mathcal{K}(L^{2}G_{\mathbb{N}})]_{G} (2.2)

is given by precomposition with the first map q​ℂ→ℂq\mathbb{C}\rightarrow\mathbb{C} as described in Section 2.1.2, see [8, Exercise 10.11.13.f]. By taking nn-fold loops on both sides of Equation 2.2, we obtain

KnG​(A)≅πn​(Hom¯G​(q​ℂ,A⊗𝒦⁡(L2​Gℕ)))K_{n}^{G}(A)\cong\pi_{n}(\underline{\operatorname{Hom}}_{G}(q\mathbb{C},A\otimes\mathcal{K}(L^{2}G_{\mathbb{N}})))

for all n∈ℕn\in\mathbb{N}.

We are now in a position to supply a concrete generator of K0C2​(𝒮)K_{0}^{C_{2}}(\mathcal{S}). To that end, we consider two distinguised C2C_{2}-invariant projections in C⁡([−1,1],M2)C([-1,1],M_{2}). Note that C⁡[−1,1]C[-1,1] with the even-odd grading is the multiplier algebra of 𝒮\mathcal{S} 1212 12 we implicitly identified 𝒮\mathcal{S} with its bounded version and M2M_{2} has the diagonal-off diagonal grading, thereby inducing the tensor product action on C⁡([−1,1],M2)C([-1,1],M_{2}). Set

p1:[−1,\displaystyle p_{1}:[-1, 1]→M2(ℂ)\displaystyle 1]\rightarrow M_{2}(\mathbb{C})
t↦(cos2⁡(π2​t)sin⁡(π2​t)​cos⁡(π2​t)sin⁡(π2​t)​cos⁡(π2​t)sin2⁡(π2​t))\displaystyle t\mapsto\begin{pmatrix}\cos^{2}(\frac{\pi}{2}t)&\sin(\frac{\pi}{2}t)\cos(\frac{\pi}{2}t)\\ \sin(\frac{\pi}{2}t)\cos(\frac{\pi}{2}t)&\sin^{2}(\frac{\pi}{2}t)\end{pmatrix}

and

p2:[−1,\displaystyle p_{2}:[-1, 1]→M2(ℂ)\displaystyle 1]\rightarrow M_{2}(\mathbb{C})
t↦(0001)\displaystyle t\mapsto\begin{pmatrix}0&0\\ 0&1\end{pmatrix}

It is clear that p1,p2p_{1},p_{2} are C2C_{2}-invariant projections in C⁡([−1,1],M2)C([-1,1],M_{2}), and that they induce a homomorphism

p1−p2:q​ℂ→M2​(𝒮)p_{1}-p_{2}:q\mathbb{C}\rightarrow M_{2}(\mathcal{S})

in the notation of Section 2.1.3.

Proposition 2.2.

The homomorphism ℤ→K0C2​(𝒮)\mathbb{Z}\rightarrow K_{0}^{C_{2}}(\mathcal{S}) given by 1↦p1−p21\mapsto p_{1}-p_{2} renders the diagram

K0C2​(𝒮){\lx@inpgf@ignorespaces{K_{0}^{C_{2}}(\mathcal{S})}}K0C2​(ℂ){\lx@inpgf@ignorespaces{K_{0}^{C_{2}}(\mathbb{C})}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}ℤ⊕ℤ{\lx@inpgf@ignorespaces{\mathbb{Z}\oplus\mathbb{Z}}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{ev}_{0}}_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}n↦(n,−n)\scriptstyle{\lx@inpgf@ignorespaces n\mapsto(n,-n)}

commutative, where the right isomorphism is the isomorphism described in Section 2.1.1.

Proof.

From the descriptions of p1p_{1} and p2p_{2} and Section 2.1, it is clear that ev0⁡(p1−p2)\operatorname{ev}_{0}(p_{1}-p_{2}) corresponds to the map q​ℂ→M2q\mathbb{C}\rightarrow M_{2} given by the difference of the C2C_{2}-equivariant projections (1000)\begin{pmatrix}1&0\\ 0&0\end{pmatrix} and (0001)\begin{pmatrix}0&0\\ 0&1\end{pmatrix} in M2M_{2}. Now, M2M_{2} with the diagonal-off diagonal grading is nothing but the algebra of operators on the C2C_{2}-vector space ℂtriv⊕ℂsign\mathbb{C}^{\operatorname{triv}}\oplus\mathbb{C}^{\operatorname{sign}}. The rest follows directly. ∎

Corollary 2.2.

The left vertical arrow above is in fact an isomorphism. We declare p:=p1−p2p:=p_{1}-p_{2} to be the preferred generator of K0C2​(𝒮)≅ℤK_{0}^{C_{2}}(\mathcal{S})\cong\mathbb{Z}.

Proof.

Since we know that K0C2​(𝒮)K_{0}^{C_{2}}(\mathcal{S}) is abstractly isomorphic to ℤ\mathbb{Z}, this follows from the elementary observation that the map

ℤ→n↦(n,−n)ℤ⊕ℤ\mathbb{Z}\xrightarrow{n\mapsto(n,-n)}\mathbb{Z}\oplus\mathbb{Z}

can only factor through ℤ\mathbb{Z} (in the category of abelian groups) through an isomorphism ℤ→ℤ\mathbb{Z}\rightarrow\mathbb{Z}. ∎

2.2 The spectral model of graded, GG-equivariant KK-theory

Recall that throughtout this subsection, GG is a compact group. We want to develop a GG-equivariant version of the spectral model of KK-theory, originally due to Higson and Guentner in the complex case ([32, Section 1.5]), and discussed with details in the Real case in [26]. The spectral model predates any ∞\infty-categorical refinements of K⁡(K)K(K)-theory, and in the present work, we would need to have formal properties of it setup a priori in order to get mileage out of the stable ∞\infty-categories for graded bivariant KK-theories constructed in Section 4 (see especially the proof of Theorem 4.4).

We begin with the relevant definitions.

Definition 2.2.

Let A∈𝖦​𝖢^∗​𝖠𝗅𝗀A\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}. Define the GG-equivariant spectral KK-theory space of AA, denoted 𝕂G,sp​(A)\mathbb{K}^{G,\operatorname{sp}}(A), to be

𝕂G,sp​(A):=Hom¯G2​(𝒮,A​⊗^​𝒦^G),\mathbb{K}^{G,\operatorname{sp}}(A):=\underline{\operatorname{Hom}}_{G_{2}}(\mathcal{S},A\hat{\otimes}\hat{\mathcal{K}}_{G}),

the G×C2G\times C_{2}-equivariant ∗*-homomorphisms from 𝒮\mathcal{S} to A​⊗^​𝒦^GA\hat{\otimes}\hat{\mathcal{K}}_{G} equipped with the point-norm topology. We define the spectral KK-theory groups of AA to be the homotopy groups of 𝕂G,sp​(A)\mathbb{K}^{G,\operatorname{sp}}(A),

KnG,sp​(A):=πn​(𝕂G,sp​(A),0¯)K_{n}^{G,\operatorname{sp}}(A):=\pi_{n}(\mathbb{K}^{G,\operatorname{sp}}(A),\underline{0})

Before studying the spectral model, we introduce the so-called Fredholm model, which formalizes the notion of GG-equivariant Fredholm operators classifying GG-equivariant KK-theory. It is also a crucial bridge between showing that the spectral model recovers the classical projective module picture of KK-theory when the algebra is inner graded.

Definition 2.2.

Let A∈𝖦​𝖢^∗​𝖠𝗅𝗀A\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}.

  • •

    A GG-Fredholm cycle over AA is a tuple (ℰ,F)(\mathcal{E},F), where ℰ\mathcal{E} is a graded, countably generated Hilbert A,GA,G-module 1313 13 see [46, Section 2.1] for the definition, and FF is a GG-continuous, GG-invariant, odd, self-adjoint Fredholm operator on it.

  • •

    Two GG-Fredholm cycles (ℰ0,F0)(\mathcal{E}_{0},F_{0}) and (ℰ1,F1)(\mathcal{E}_{1},F_{1}) over AA are said to be concordant if there exists a GG-Fredholm cycle (ℰ,F)(\mathcal{E},F) over A​⊗^​C​[0,1]≅C⁡([0,1],A)A\hat{\otimes}C[0,1]\cong C([0,1],A) such that (ℰ​⊗^evi​A,evi⁡(F))≅(ℰi,Fi)(\mathcal{E}\hat{\otimes}_{\operatorname{ev}_{i}}A,\operatorname{ev}_{i}(F))\cong(\mathcal{E}_{i},F_{i}) for i=0,1i=0,1, where evt:C⁡([0,1],A)→A\operatorname{ev}_{t}:C([0,1],A)\rightarrow A is the homomorphism given by evt⁡(f)=f⁡(t)\operatorname{ev}_{t}(f)=f(t).

  • •

    Denote by K0G,Fr​(A)K_{0}^{G,\operatorname{Fr}}(A) the abelian monoid of concordance classes of GG-Fredholm cycles over AA.

Theorem 2.3.

Some key features of the spectral model and the Fredholm model of graded, GG-equivariant KK-theory are mentioned below. In what follows, A,B,…A,B,... denote arbitrary graded GG-C∗C^{*}-algebras, and all the morphisms are in the category 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}.

  1. 1.

    𝕂G,sp​(A)\mathbb{K}^{G,\operatorname{sp}}(A) is an HH-group. Consequently, all the equivariant spectral KK-groups are in fact abelian groups.

  2. 2.

    A short exact sequence 0→A→B→C→00\rightarrow A\rightarrow B\rightarrow C\rightarrow 0 in 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg} yields a Serre fibration on the associated spectral KK-theory spaces.

  3. 3.

    The functors KnG,sp​(−):𝖦​𝖢^∗​𝖠𝗅𝗀→AbK_{n}^{G,\operatorname{sp}}(-):\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}\rightarrow\operatorname{Ab} preserve filtered colimits for all n∈ℕ≥0n\in\mathbb{N}_{\geq 0}.

  4. 4.

    The functors

    K0G,sp(−):(𝖦𝖢^∗𝖠𝗅𝗀,⊗^!)→(Ab,⊗)K_{0}^{G,\operatorname{sp}}(-):(\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg},\hat{\otimes}_{!})\rightarrow(\operatorname{Ab},\otimes)

    are lax monoidal.

  5. 5.

    We have a natural isomorphism of abelian groups

    π0​(𝕂G,sp​(A))→≅K0G,Fr​(A).\pi_{0}(\mathbb{K}^{G,\operatorname{sp}}(A))\xrightarrow{\cong}K_{0}^{G,\operatorname{Fr}}(A).
  6. 6.

    When AA is inner graded, we have a natural isomorphism of abelian groups

    πn​(𝕂G,sp​(A))≅KnG​(A)​∀n≥0.\pi_{n}(\mathbb{K}^{G,\operatorname{sp}}(A))\cong K_{n}^{G}(A)\penalty\ \forall\penalty\ n\geq 0.
Proof sketch.

Assertion 1 follows from the more general statement that given a graded morphism φ:𝒮→A\varphi:\mathcal{S}\rightarrow A, the induced morphism

𝒮→A​⊗^​M2​(ℂ)=M2​(A),f↦(φ⁡(f)00α⁡(φ⁡(f)))\mathcal{S}\rightarrow A\hat{\otimes}M_{2}(\mathbb{C})=M_{2}(A),\penalty\ \penalty\ \penalty\ f\mapsto\begin{pmatrix}\varphi(f)&0\\ 0&\alpha(\varphi(f))\end{pmatrix}

is nullhomotopic in Hom¯G​(𝒮,A​⊗^​M2​(ℂ))\underline{\operatorname{Hom}}_{G}(\mathcal{S},A\hat{\otimes}M_{2}(\mathbb{C})) (here α\alpha is the grading on AA), where M2​(ℂ)M_{2}(\mathbb{C}) has the grading given by Ad⁡(τ)\operatorname{Ad}(\tau), where τ=(100−1)\tau=\begin{pmatrix}1&0\\ 0&-1\end{pmatrix}. See [32, Remark 1.7].

Assertion 2 follows from the non-equivariant assertion proven in [26, Section 3.2] by taking GG-fixed points. Note that taking GG-fixed points is an exact functor because GG is compact.

By similar reductions as done before, to show Assertion 3, it suffices to prove that for a filtered diagram (Ai)i∈I(A_{i})_{i\in I} of non-equivariant graded C∗C^{*}-algebras with colimit AA, one has a weak homotopy equivalence of spaces

colimi∈I⁡Hom¯​(𝒮,Ai)→Hom¯​(𝒮,A).\operatorname{colim}_{i\in I}\underline{\operatorname{Hom}}(\mathcal{S},A_{i})\rightarrow\underline{\operatorname{Hom}}(\mathcal{S},A).

Upon passing to the Cayley transform picture (see [26, Lemma 3.1]), the result follows from [48, Corollary to Theorem 12].

The key to demonstrating Assertion 4 is the comultiplication map on 𝒮\mathcal{S} as described in [26, Section 4.2]. The details are in [26, Section 6], and the same proofs go through equivariantly. See also Section 4.

We now discuss Assertion 5. A natural map π0​(𝕂G,sp​(A))→≅K0G,Fr​(A)\pi_{0}(\mathbb{K}^{G,\operatorname{sp}}(A))\xrightarrow{\cong}K_{0}^{G,\operatorname{Fr}}(A) can be written by directly emulating the non-equivariant construction as in [26, Section 8.5]. We mention some aspects of it for ease of reference later.

Firstly, we implicitly replace 𝒮\mathcal{S} with 𝒮~\tilde{\mathcal{S}}, and the Fredholm cycles with essentially unitary ones. Recall that

A​⊗^​𝒦^G≅𝒦A​(A⊗L2​Gℕ^),A\hat{\otimes}\hat{\mathcal{K}}_{G}\cong\mathcal{K}_{A}(A\otimes\widehat{L^{2}G_{\mathbb{N}}}),

the GG-equivariant graded C∗C^{*}-algebra of AA-compact operators on the standard graded GG-equivariant Hilbert AA-module. Given φ:𝒮→A​⊗^​𝒦^G≅𝒦A​(A⊗L2​Gℕ^)\varphi:\mathcal{S}\rightarrow A\hat{\otimes}\hat{\mathcal{K}}_{G}\cong\mathcal{K}_{A}(A\otimes\widehat{L^{2}G_{\mathbb{N}}}), set

ℋφ:=φ​(𝒮)​(A⊗L2​Gℕ^)¯,\mathcal{H}_{\varphi}:=\overline{\varphi(\mathcal{S})(A\otimes\widehat{L^{2}G_{\mathbb{N}}})},

and note that φ\varphi restricts to a non-degenerate homomorphism

φnd:𝒮→𝒦A​(ℋφ).\varphi^{\operatorname{nd}}:\mathcal{S}\rightarrow\mathcal{K}_{A}(\mathcal{H}_{\varphi}).

The crucial point here is that φnd\varphi^{\operatorname{nd}} indeed maps to the AA-compact operators on the (not necessarily complementable) submodule ℋφ⊆A⊗L2​Gℕ^\mathcal{H}_{\varphi}\subseteq A\otimes\widehat{L^{2}G_{\mathbb{N}}}, as is guaranteed by [46, Lemma 4.1]. Non-degeneracy of φnd\varphi^{\operatorname{nd}} implies that there exists a unique GG-equivariant, graded homomorphism φ~:C⁡[−1,1]→ℬ⁡(ℋφ)\tilde{\varphi}:C[-1,1]\rightarrow\mathcal{B}(\mathcal{H}_{\varphi}) extending φnd\varphi^{\operatorname{nd}}. The natural map is now given by

π0​(𝕂G,sp​(A))→\displaystyle\pi_{0}(\mathbb{K}^{G,\operatorname{sp}}(A))\xrightarrow{} K0G,Fr​(A)\displaystyle K_{0}^{G,\operatorname{Fr}}(A)
φ⟼\displaystyle\varphi\longmapsto (ℋφ,φ~​(x))\displaystyle(\mathcal{H}_{\varphi},\tilde{\varphi}(x))

The proof that this map is bijective now follows with the obvious modifications from [26, Section 8.5].

Finally, we come to Assertion 6. We just discuss the case of π0\pi_{0} when AA is unital and ungraded, the general case follows from the techniques described in [63, Section 2.9]. One proof strategy in the unital, ungraded case would be to show that the natural map K0G​(A)→K0G,Fr​(A)K_{0}^{G}(A)\rightarrow K_{0}^{G,\operatorname{Fr}}(A) has an inverse given by taking the GG-equivariant index of GG-invariant Fredholm operators (as done in the non-equivariant case in [26, Section 8.4]), and then conclude by Assertion 5. However, granted the results of loc.​ cit.​ and the Green-Julg theorem, we can quickly obtain the conclusion by leveraging the fact that A⋊G≅(A⊗𝒦⁡(L2​G))GA\rtimes G\cong(A\otimes\mathcal{K}(L^{2}G))^{G}, as shown in [29, Proposition 11.2]. See also the proof of [27, Proposition 3.1]. ∎

Notation 2.3.

Having established natural isomorphisms between different models of graded KK-theory, we henceforth denote the GG-equivariant graded KK-groups as K^∗G​(−)\hat{K}^{G}_{*}(-).

Next, we analyse the graded K0K_{0}-group of 𝒮\mathcal{S} (ignoring the external group GG). We summarize our results in the following proposition. Note that all the algebras C0​(ℝn)C_{0}(\mathbb{R}^{n}) in the below proof (and in general) carry the trivial grading. The author learnt most of these results from Johannes Ebert.

Proposition 2.3.
  1. 1.

    There is a short exact sequence

    0→C0​(ℝ)​⊗^​C​l0,1→𝜓𝒮→ev0ℂ→00\xrightarrow{}C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\xrightarrow{\psi}\mathcal{S}\xrightarrow{\operatorname{ev}_{0}}\mathbb{C}\rightarrow 0

    in 𝖢^∗​𝖠𝗅𝗀\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}.

  2. 2.

    For every A∈𝖢^∗​𝖠𝗅𝗀A\in\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}, the map

    Hom¯​(𝒮,𝒮​⊗^​A)→(ev0⁡⊗^​1A)∗Hom¯​(𝒮,A)\underline{\operatorname{Hom}}(\mathcal{S},\mathcal{S}\hat{\otimes}A)\xrightarrow{(\operatorname{ev}_{0}\hat{\otimes}1_{A})_{*}}\underline{\operatorname{Hom}}(\mathcal{S},A)

    have natural continuous sections σA\sigma_{A}. Furthermore, σℂ​(ev0)=1𝒮\sigma_{\mathbb{C}}(\operatorname{ev}_{0})=\operatorname{1}_{\mathcal{S}}.

  3. 3.

    For every A∈𝖢^∗​𝖠𝗅𝗀A\in\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}, we have naturally split exact sequences

    0→K^∗​(C0​(ℝ)​⊗^​C​l0,1​⊗^​A)→ψ∗K^∗​(𝒮​⊗^​A)→ev0∗K^∗​(A)→0.0\rightarrow\hat{K}_{*}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\hat{\otimes}A)\xrightarrow{\psi_{*}}\hat{K}_{*}(\mathcal{S}\hat{\otimes}A)\xrightarrow{\operatorname{{ev}_{0}}_{*}}\hat{K}_{*}(A)\rightarrow 0.
  4. 4.

    For each n∈ℕn\in\mathbb{N}, multiplication by the Bott class [βℂn]∈K^​(C0​(ℝn)​⊗^​C​l0,n)[\beta_{\mathbb{C}}^{n}]\in\hat{K}(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}) yields natural isomorphisms

    K^∗​(A)→K^∗​(C0​(ℝn)​⊗^​C​l0,n​⊗^​A).\hat{K}_{*}(A)\rightarrow\hat{K}_{*}(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}\hat{\otimes}A).

    In particular, K^0​(C0​(ℝn)​⊗^​C​l0,n)≅ℤ\hat{K}_{0}(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n})\cong\mathbb{Z}, and the isomorphism identifies [βℂn][\beta_{\mathbb{C}}^{n}] and 11. The grading α\alpha on C0​(ℝn)​⊗^​C​l0,nC_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n} induces the map (−1)n:ℤ→ℤ(-1)^{n}:\mathbb{Z}\rightarrow\mathbb{Z}.

  5. 5.

    K^0​(𝒮)≅ℤ⊕ℤ\hat{K}_{0}(\mathcal{S})\cong\mathbb{Z}\oplus\mathbb{Z} as abelian groups, with the preferred isomorphism mapping ψ∗​[βℂ]=:u\psi_{*}[\beta_{\mathbb{C}}]=:u to (0,1)(0,1) and [1𝒮]=:e[\operatorname{1_{\mathcal{S}}}]=:e to (1,0)(1,0).

  6. 6.

    The composition

    C0​(ℝ)​⊗^​C​l0,1→𝜓𝒮→βℂC0​(ℝ)​⊗^​C​l0,1C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\xrightarrow{\psi}\mathcal{S}\xrightarrow{\beta_{\mathbb{C}}}C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}

    induces multiplication by 22 on K^0​(C0​(ℝ)​⊗^​C​l0,1)≅ℤ\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})\cong\mathbb{Z}.

  7. 7.

    In the context of Assertion 5, we have α∗​(u)=−u\alpha_{*}(u)=-u and α∗​(e)=e−u\alpha_{*}(e)=e-u, where α\alpha denotes the grading on 𝒮\mathcal{S}.

  8. 8.

    There exists an isomorphism of C2C_{2}-abelian groups between K0^​(𝒮)\hat{K_{0}}(\mathcal{S}) and ℤ⊕ℤ\mathbb{Z}\oplus\mathbb{Z} with the flip action, with the preferred isomorphism sending [1𝒮][1_{\mathcal{S}}] to (1,0)(1,0) and [α𝒮][\alpha_{\mathcal{S}}] to (0,1)(0,1).

Proof.

We begin with Assertion 1. Consider

0→J→𝒮→ev0ℂ→00\xrightarrow{}J\xrightarrow{}\mathcal{S}\xrightarrow{\operatorname{ev}_{0}}\mathbb{C}\rightarrow 0

where J:=ker⁡(ev0)J:=\ker(\operatorname{ev}_{0}). Then, we have

J→≅C0​((0,∞))​⊗^​C​l0,1f↦fev∣(0,∞)​⊗^​1+fodd∣(0,∞)​⊗^​ε,\displaystyle J\xrightarrow{\cong}C_{0}((0,\infty))\hat{\otimes}Cl^{0,1}\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ f\mapsto f_{\operatorname{ev}}\mid_{(0,\infty)}\hat{\otimes}1+f_{\operatorname{odd}}\mid_{(0,\infty)}\hat{\otimes}\varepsilon, (2.4)

where fev​(x)=f⁡(x)+f⁡(−x)2,fodd​(x)=f⁡(x)−f⁡(−x)2f_{\operatorname{ev}}(x)=\frac{f(x)+f(-x)}{2},f_{{\operatorname{odd}}}(x)=\frac{f(x)-f(-x)}{2}, and ε\varepsilon is the canonical generator of C​l0,1Cl^{0,1}. Take a homeomorphism h:(0,∞)→ℝh:(0,\infty)\rightarrow\mathbb{R} such that

limt→0h⁡(t)=−∞,limt→∞h⁡(t)=∞.\lim_{t\to 0}h(t)=-\infty,\lim_{t\to\infty}h(t)=\infty.

For concreteness, take h⁡(x)=ln⁡(x)h(x)=\ln(x). We can define our sought after map ψ:C0​(ℝ)​⊗^​C​l0,1→𝒮\psi:C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\rightarrow\mathcal{S} using hh and the isomorphism above.

For Assertion 2, note that a direct calculation using the generators e−x2e^{-x^{2}} and x​e−x2xe^{-x^{2}} of 𝒮\mathcal{S} shows that the composite

Hom⁡(𝒮,A)→1𝒮​⊗^−Hom⁡(𝒮​⊗^​𝒮,𝒮​⊗^​A)→Δ∗Hom⁡(𝒮,𝒮​⊗^​A)→(ev0⁡⊗^​1A)∗Hom⁡(𝒮,A)\operatorname{Hom}(\mathcal{S},A)\xrightarrow{1_{\mathcal{S}}\hat{\otimes}-}\operatorname{Hom}(\mathcal{S}\hat{\otimes}\mathcal{S},\mathcal{S}\hat{\otimes}A)\xrightarrow{\Delta^{*}}\operatorname{Hom}(\mathcal{S},\mathcal{S}\hat{\otimes}A)\xrightarrow{(\operatorname{ev}_{0}\hat{\otimes}1_{A})_{*}}\operatorname{Hom}(\mathcal{S},A)

is the identity, and has the required effect on ev0∈Hom⁡(𝒮,ℂ)\operatorname{ev}_{0}\in\operatorname{Hom}(\mathcal{S},\mathbb{C}) too.

Assertion 3 follows immediately from Assertion 2.

We just prove the last part of Assertion 4, since the first two parts are the content of [26, Section 9]. Recall that the Bott class is the class in graded KK-theory represented by the Bott map, which is the functional calculus of the embedding of ℝn\mathbb{R}^{n} in C​l0,n{Cl^{0,n}} as a homomorphism 𝒮→C0​(ℝn,C​l0,n)\mathcal{S}\rightarrow C_{0}(\mathbb{R}^{n},Cl^{0,n}).1515 15 strictly speaking, we mean ℝ0,n\mathbb{R}^{0,n} here

We begin with the case n=1n=1. To simplify the notation, we denote βℂ1\beta_{\mathbb{C}}^{1} by βℂ\beta_{\mathbb{C}}. We have to show that α∗​([βℂ])=−[βℂ]\alpha_{*}([\beta_{\mathbb{C}}])=-[\beta_{\mathbb{C}}]. By definition of βℂ\beta_{\mathbb{C}}, we have

βℂ:𝒮\displaystyle\beta_{\mathbb{C}}:\mathcal{S} →C0​(ℝ)​⊗^​C​l0,1≅C0​(ℝ,C​l0,1)f↦t↦f⁡(t​ε).\displaystyle\rightarrow C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\cong C_{0}(\mathbb{R},Cl^{0,1})\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ f\mapsto t\mapsto f(t\varepsilon).

This is same as the map f↦fev+fodd​εf\mapsto f^{\operatorname{ev}}+f^{\operatorname{odd}}\varepsilon, as can be readily checked on the generators uu and vv of 𝒮\mathcal{S}. Therefore, we have

α∘βℂ:𝒮\displaystyle\alpha\circ\beta_{\mathbb{C}}:\mathcal{S} →C0​(ℝ,C​l0,1),f↦fev−fodd​ε.\displaystyle\rightarrow C_{0}(\mathbb{R},Cl^{0,1}),\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ f\mapsto f^{\operatorname{ev}}-f^{\operatorname{odd}}\varepsilon.

We now identify

Hom⁡(𝒮,C0​(ℝ)​⊗^​C​l0,1)≅Map∗⁡(ℝ+,Hom⁡(𝒮,C​l0,1)).\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})\cong\operatorname{Map}_{*}(\mathbb{R}^{+},\operatorname{Hom}(\mathcal{S},Cl^{0,1})).

Furthermore, under the Cayley transform isomorphism, we have a homeomorphism1616 16 in what follows, we denote by ℝ+\mathbb{R}^{+} the one-point compactification of ℝ\mathbb{R}. ∞∈ℝ+\infty\in\mathbb{R}^{+} is the point at infinity.

ℝ+\displaystyle\mathbb{R}^{+} →Hom⁡(𝒮,C​l0,1)\displaystyle\rightarrow\operatorname{Hom}(\mathcal{S},Cl^{0,1}) (2.5)
∞\displaystyle\infty ↦0\displaystyle\mapsto 0 (2.6)
t\displaystyle t ⟼f↦fev​(t)+fodd​(t)​ε\displaystyle\longmapsto f\mapsto f^{\operatorname{ev}}(t)+f^{\operatorname{odd}}(t)\varepsilon (2.7)

Whence, we have a homeomorphism of spaces

Hom⁡(𝒮,C0​(ℝ)​⊗^​C​l0,1)≅Map∗⁡(ℝ+,ℝ+),\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})\cong\operatorname{Map}_{*}(\mathbb{R}^{+},\mathbb{R}^{+}),

under which βℂ\beta_{\mathbb{C}} corresponds to the identity, and α∘β\alpha\circ\beta corresponds to the negative of identity. Since degree of the negative identity as a map from ℝ+\mathbb{R}^{+} to itself is −1-1, the conclusion follows.

For the general case, we consider the commutative diagram of abelian groups (see [26, Section 7.1] for the details)

K^0​(C0​(ℝ)​⊗^​C​l0,1)⊗K^0​(C0​(ℝ)​⊗^​C​l0,1)⊗⋯⊗K^0​(C0​(ℝ)​⊗^​C​l0,1)⟶K^0​(C0​(ℝn)​⊗^​C​l0,n)↓α∗↓α∗↓α∗↓α∗K^0​(C0​(ℝ)​⊗^​C​l0,1)⊗K^0​(C0​(ℝ)​⊗^​C​l0,1)⊗⋯⊗K^0​(C0​(ℝ)​⊗^​C​l0,1)⟶K^0​(C0​(ℝn)​⊗^​C​l0,n).\begin{array}[]{ccccccc}\hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\otimes&\hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\otimes\cdots\otimes&\hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\longrightarrow&\hat{K}_{0}\!\left(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}\right)\\[4.30554pt] \downarrow\!{\scriptstyle\alpha_{*}}&&\downarrow\!{\scriptstyle\alpha_{*}}&&\downarrow\!{\scriptstyle\alpha_{*}}&&\downarrow\!{\scriptstyle\alpha_{*}}\\[4.30554pt] \hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\otimes&\hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\otimes\cdots\otimes&\hat{K}_{0}\!\left(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\right)&\longrightarrow&\hat{K}_{0}\!\left(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}\right).\end{array}

From [63, Lemma 9.3.4] on the one hand we get

[βℂ]×[βℂ]×…×[βℂ]↦[βℂn]∈K^0​(C0​(ℝn)​⊗^​C​l0,n).[\beta_{\mathbb{C}}]\times[\beta_{\mathbb{C}}]\times...\times[\beta_{\mathbb{C}}]\mapsto[\beta_{\mathbb{C}}^{n}]\in\hat{K}_{0}(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}).

Since α∗​([βℂ])=−[βℂ]\alpha_{*}([\beta_{\mathbb{C}}])=-[\beta_{\mathbb{C}}] for the case dealt with above, from the commutativity of the above diagram, we get on the other hand

(−[βℂ])×(−[βℂ])×…×(−[βℂ])↦α∗​[βℂn]∈K^0​(C0​(ℝn)​⊗^​C​l0,n).(-[\beta_{\mathbb{C}}])\times(-[\beta_{\mathbb{C}}])\times...\times(-[\beta_{\mathbb{C}}])\mapsto\alpha_{*}[\beta_{\mathbb{C}}^{n}]\in\hat{K}_{0}(C_{0}(\mathbb{R}^{n})\hat{\otimes}Cl^{0,n}).

This proves Assertion 4.

Assertion 5 follows immediately from Assertions 3 and 4.

We now show Assertion 6. Choose a homeomorphism h:(0,∞)→ℝh:(0,\infty)\rightarrow\mathbb{R} as in the proof of Assertion 1. By definition, the composition βℂ∘ψ\beta_{\mathbb{C}}\circ\psi is

C0​(ℝ)​⊗^​C​l0,1→h∗C0​((0,∞))​⊗^​C​l0,1→𝒮→βℂC0​(ℝ)​⊗^​C​l0,1,C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}\xrightarrow{h^{*}}C_{0}((0,\infty))\hat{\otimes}Cl^{0,1}\xrightarrow{}\mathcal{S}\xrightarrow{\beta_{\mathbb{C}}}C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1},

where the unlabelled arrow sends

f​⊗^​1⟼x↦f⁡(|x|),f​⊗^​ε⟼x↦s⁡(x)​f​(|x|),f\hat{\otimes}1\longmapsto x\mapsto f(|x|),\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ f\hat{\otimes}\varepsilon\longmapsto x\mapsto s(x)f(|x|),

where s⁡(x):ℝ∖{0}→{−1,1}s(x):\mathbb{R}\setminus\{0\}\rightarrow\{-1,1\} is the sign function1717 17 strictly speaking these are the formulae when x≠0x\neq 0. At x=0x=0 we by default assign the value 00. We also do this at certain places later without explicitly mentioning. (this function is nothing but the inverse to the isomorphism in Equation 2.4 postcomposed with the inclusion of JJ into 𝒮\mathcal{S}). The whole composite therefore sends

f⊗^1⟼f∘h∘|⋅|⊗^1,f⊗^ε⟼(s⋅f∘h∘|⋅|)⊗^ε.f\hat{\otimes}1\longmapsto f\circ h\circ|\cdot|\hat{\otimes}1,\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ f\hat{\otimes}\varepsilon\longmapsto(s\cdot f\circ h\circ|\cdot|)\hat{\otimes}\varepsilon.

From the description of the Bott map as in the proof of Assertion 4, the induced map

Hom⁡(𝒮,C0​(ℝ)​⊗^​C​l0,1)\displaystyle\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}) →(βℂ∘ψ)∗Hom⁡(𝒮,C0​(ℝ)​⊗^​C​l0,1)\displaystyle\xrightarrow{(\beta_{\mathbb{C}}\circ\psi)_{*}}\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})

sends the Bott map to the homomorphism

(f⟼fev∘h∘|⋅|)⊗^1+(s⋅fodd∘h∘|⋅|)⊗^ε.(f\longmapsto f^{\operatorname{ev}}\circ h\circ|\cdot|)\hat{\otimes}1+(s\cdot f^{\operatorname{odd}}\circ h\circ|\cdot|)\hat{\otimes}\varepsilon.

Upon identifying

Hom⁡(𝒮,C0​(ℝ)​⊗^​C​l0,1)≅Map∗⁡(ℝ+,Hom⁡(𝒮,C​l0,1)),\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})\cong\operatorname{Map}_{*}(\mathbb{R}^{+},\operatorname{Hom}(\mathcal{S},Cl^{0,1})),

the Bott map therefore gets mapped to

x⟼f↦(fev​(h⁡(|x|))⋅1+s⁡(x)​fodd​(h⁡(|x|))⋅ε).x\longmapsto f\mapsto(f^{\operatorname{ev}}(h(|x|))\cdot 1+s(x)f^{\operatorname{odd}}(h(|x|))\cdot\varepsilon).

But this is same as the function

ℝ+\displaystyle\mathbb{R}^{+} →Hom⁡(𝒮,C​l0,1)\displaystyle\rightarrow\operatorname{Hom}(\mathcal{S},Cl^{0,1})
x\displaystyle x ⟼f↦{fev​(h⁡(x))⋅1+fodd​(h⁡(x))⋅εif​x>0fev​(h⁡(−x))⋅1−fodd​(h⁡(−x))⋅εif​x<00if​x=0,∞\displaystyle\longmapsto f\mapsto\begin{cases}f^{\operatorname{ev}}(h(x))\cdot 1+f^{\operatorname{odd}}(h(x))\cdot\varepsilon\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \text{if}\penalty\ x>0\\ f^{\operatorname{ev}}(h(-x))\cdot 1-f^{\operatorname{odd}}(h(-x))\cdot\varepsilon\penalty\ \penalty\ \penalty\ \penalty\ \text{if}\penalty\ x<0\\ 0\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \text{if}\penalty\ x=0,\infty\end{cases}

Under the identification

ℝ+≅Hom⁡(𝒮,C​l0,1)\mathbb{R}^{+}\cong\operatorname{Hom}(\mathcal{S},Cl^{0,1})

from Equation 2.5, this corresponds to the function

h′:ℝ+\displaystyle h^{\prime}:\mathbb{R}^{+} →ℝ+\displaystyle\rightarrow\mathbb{R}^{+}
x\displaystyle x ↦{h⁡(x)​if​x>0−h⁡(−x)​if​x<0∞if​x=0,∞\displaystyle\mapsto\begin{cases}h(x)\penalty\ \text{if}\penalty\ x>0\\ -h(-x)\penalty\ \text{if}\penalty\ x<0\\ \infty\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \text{if}\penalty\ x=0,\infty\end{cases}

The local degree formula yields that the degree of h′h^{\prime} is 22. The proof is now completed by the following argument: consider the diagram

Hom⁡(𝒮,C0​(ℝ,C​l0,1)){\lx@inpgf@ignorespaces{\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R},Cl^{0,1}))}}Hom⁡(𝒮,C0​(ℝ,C​l0,1)){\lx@inpgf@ignorespaces{\operatorname{Hom}(\mathcal{S},C_{0}(\mathbb{R},Cl^{0,1}))}}Map∗⁡(ℝ+,Hom⁡(𝒮,C​l0,1)){\lx@inpgf@ignorespaces{\operatorname{Map}_{*}(\mathbb{R}^{+},\operatorname{Hom}(\mathcal{S},Cl^{0,1}))}}Map∗⁡(ℝ+,Hom⁡(𝒮,C​l0,1)){\lx@inpgf@ignorespaces{\operatorname{Map}_{*}(\mathbb{R}^{+},\operatorname{Hom}(\mathcal{S},Cl^{0,1}))}}Map∗⁡(ℝ+,ℝ+){\lx@inpgf@ignorespaces{\operatorname{Map}_{*}(\mathbb{R}^{+},\mathbb{R}^{+})}}Map∗⁡(ℝ+,ℝ+),{\lx@inpgf@ignorespaces{\operatorname{Map}_{*}(\mathbb{R}^{+},\mathbb{R}^{+})},}(βℂ∘ψ)∗\scriptstyle{\lx@inpgf@ignorespaces(\beta_{\mathbb{C}}\circ\psi)_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}

where the bottom horizontal arrow is defined so as to make the diagram commute. Therefore the bottom horizontal arrow sends

id:ℝ+→ℝ+\operatorname{id}:\mathbb{R}^{+}\rightarrow\mathbb{R}^{+}

to

h′:ℝ+→ℝ+,h^{\prime}:\mathbb{R}^{+}\rightarrow\mathbb{R}^{+},

since we showed above that the right-down itinerary maps βℂ\beta_{\mathbb{C}} to h′h^{\prime}, and the left vertical composite identifies βℂ\beta_{\mathbb{C}} and id\operatorname{id}, as was observed in the proof of Assertion 4. Thus, the map induced by βℂ∘ψ\beta_{\mathbb{C}}\circ\psi on K^0​(C0​(ℝ,C​l0,1))\hat{K}_{0}(C_{0}(\mathbb{R},Cl^{0,1})) is multiplication by the degree of h′h^{\prime}, which is equal to 22.

For Assertion 7, we consider the commutative diagram (we denote by α\alpha the grading on the respective algebras)

0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}K^0​(C0​(ℝ)​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})}}K^0​(C0​(ℝ)​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})}}K^0​(𝒮){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathcal{S})}}K^0​(𝒮){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathcal{S})}}K0^​(ℂ){\lx@inpgf@ignorespaces{\hat{K_{0}}(\mathbb{C})}}K^0​(ℂ){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathbb{C})}}0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}α∗=−1.\scriptstyle{\lx@inpgf@ignorespaces\alpha_{*}=-1.}ψ∗\scriptstyle{\lx@inpgf@ignorespaces\psi_{*}}ψ∗\scriptstyle{\lx@inpgf@ignorespaces\psi_{*}}α∗\scriptstyle{\lx@inpgf@ignorespaces\alpha_{*}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{ev}_{0}}_{*}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces{\operatorname{ev}_{0}}_{*}}α∗=1.\scriptstyle{\lx@inpgf@ignorespaces\alpha_{*}=1.}

where the the top horizontal map is negation from Assertion 4, and the bottom horizontal map is the identity since ℂ\mathbb{C} has the trivial grading. The commutativity of the top rectangle yields that

α∗​(u)=−u.\alpha_{*}(u)=-u.

Understanding α∗​(e)\alpha_{*}(e) takes a bit more work. From Assertion 5 and the commutativity of the lower rectangle in the above diagram, we can say that

α∗​(e)=e+n​u\alpha_{*}(e)=e+nu

for some n∈ℤn\in\mathbb{Z}. To compute the value of nn, we consider the commutative diagram

K^0​(𝒮){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathcal{S})}}K^0​(𝒮){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathcal{S})}}K^0​(C0​(ℝ)​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})}}K^0​(C0​(ℝ)​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1})}}α∗\scriptstyle{\lx@inpgf@ignorespaces\alpha_{*}}β∗\scriptstyle{\lx@inpgf@ignorespaces\beta_{*}}β∗\scriptstyle{\lx@inpgf@ignorespaces\beta_{*}}α∗=−1.\scriptstyle{\lx@inpgf@ignorespaces\alpha_{*}=-1.}

From Assertion 4 and Assertion 6, we can say that β∗​(e)=[βℂ]\beta_{*}(e)=[\beta_{\mathbb{C}}] and β∗​(u)=2​[βℂ]\beta_{*}(u)=2[\beta_{\mathbb{C}}]. Tracing the fate of ee under the two itineraries from K^0​(𝒮)\hat{K}_{0}(\mathcal{S}) to K^0​(C0​(ℝ)​⊗^​C​l0,1)\hat{K}_{0}(C_{0}(\mathbb{R})\hat{\otimes}Cl^{0,1}), we obtain the equation

[βℂ]+2​n⋅[βℂ]=−[βℂ],[\beta_{\mathbb{C}}]+2n\cdot[\beta_{\mathbb{C}}]=-[\beta_{\mathbb{C}}],

which shows

n=−1.n=-1.

This finishes the proof of Assertion 7.

To prove Assertion 8, we note that Assertion 7 shows (in light of Assertion 5) that (e,α∗​e)(e,\alpha_{*}e) is also a ℤ\mathbb{Z}-basis of K^0​(𝒮)\hat{K}_{0}(\mathcal{S}), and the grading α𝒮\alpha_{\mathcal{S}} evidently swaps the basis elements. ∎

3 Equivariant (ungraded) Real KK!KK_{!}-theory

Throughout this section, we work with Real C∗C^{*}-algebras as always. Recall that !∈{se,ex}!\in\{\operatorname{se,ex}\} denotes the type of excision we have in our bivariant KK-theory, where se\operatorname{se} stands for semi-split and ex\operatorname{ex} stands for exact. In the remainder of this article, we use the superscript “sep” to denote separable versions of the categories described in Section 2.

In this section, we will first define a small stable ∞\infty-category KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} as a series of Dwyer-Kan localizations of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. Then, we take ind-completions to get a presentable, stable ∞\infty-category KKG!,∞\mathrm{KK}^{G}_{!,\infty} together with a universal functor 𝖦𝖢∗𝖠𝗅𝗀→KKG!,∞\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\mathrm{KK}^{G}_{!,\infty}. We devote the next few subsections to analyzing each step of the localization. Before proceeding, we remind the readers that 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is an essentially small category.

3.1 Inverting homotopy equivalences

In the first step, we perform the Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} at the class of (GG-equivariant) homotopy equivalences. We begin by recalling the relevant definitions.

Definition 3.0.
  1. 1.

    Two maps f0,f1:A→Bf_{0},f_{1}:A\rightarrow B in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} are said to be homotopic if there exists a morphism F:A→C⁡([0,1],B)F:A\rightarrow C([0,1],B) such that evi∘F=fi\operatorname{ev}_{i}\circ F=f_{i} for i=0,1i=0,1.

  2. 2.

    Let f:A→Bf:A\rightarrow B be a morphism in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. ff is said to be a homotopy equivalence if there exists a morphism g:B→Ag:B\rightarrow A in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} such that the two composites are homotopic to the respective identity maps.

We denote by 𝒲h\mathcal{W}_{h} the (essentially small) class of homotopy equivalences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

Definition 3.0.

Denote by 𝖦𝖢∗​𝖠𝗅𝗀hsep{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}} the Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} at 𝒲h\mathcal{W}_{h}, and denote by

Lh:𝖦𝖢∗​𝖠𝗅𝗀sep→𝖦𝖢∗​𝖠𝗅𝗀hsepL_{h}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}

the localization functor.

By definition, this means for any ∞\infty-category 𝒟\mathcal{D}, we have an equivalence of functor categories

𝐅𝐮𝐧⁡(𝖦𝖢∗​𝖠𝗅𝗀hsep,𝒟)→≃Lh∗𝐅𝐮𝐧h​(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h}^{*}}\mathbf{Fun}^{h}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}), (3.1)

where the right-hand side denotes the full subcategory of 𝐅𝐮𝐧⁡(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟)\mathbf{Fun}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}) spanned by functors which sends homotopy equivalences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to equivalences in 𝒟\mathcal{D}.

To phrase the relevant properties of the ∞\infty-category 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}, we need the notion of Schochet fibrations, defined first in [52]. Recall that the category 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is topological enriched, as mentioned in Section 2. Although it is not necessary for us, the basic definitions and properties of Schochet fibrations also work verbatim in the category 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}.

Definition 3.1.
  1. 1.

    A morphism f:A→Bf:A\rightarrow B in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is said to be a Schochet fibration if for all D∈𝖦𝖢∗​𝖠𝗅𝗀sepD\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the induced map of topological spaces

    Hom¯​(D,A)→f∗Hom¯​(D,B)\underline{\operatorname{Hom}}(D,A)\xrightarrow{f_{*}}\underline{\operatorname{Hom}}(D,B)

    is a Serre fibration.

  2. 2.

    A cartesian square in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}

    A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}D{\lx@inpgf@ignorespaces D}C{\lx@inpgf@ignorespaces C}f\scriptstyle{\lx@inpgf@ignorespaces f}

    is called Schochet fibrant if ff is a Schochet fibration.

  3. 3.

    For an ∞\infty-category 𝒟\mathcal{D}, a functor 𝖦𝖢∗​𝖠𝗅𝗀sep→𝒟\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathcal{D} will be called Schochet exact if it maps Schochet fibrant cartesian squares to cartesian squares. We denote by

    𝐅𝐮𝐧S​c​h​(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟)\mathbf{Fun}^{Sch}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D})

    the full subcategory of 𝐅𝐮𝐧⁡(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟)\mathbf{Fun}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}) spanned by functors which are Schochet exact.

Example 3.1.

We present a few important examples of Schochet fibrations which will be required later on. For proofs see the relevant sections in [52] and [17].

  1. 1.

    For any C∗C^{*}-algebra AA, the canonical map C⁡([0,1],A)→ev0AC([0,1],A)\xrightarrow{\operatorname{ev}_{0}}A is a Schochet fibration (and a homotopy equivalence). C⁡([0,1],A)C([0,1],A) is also called the path algebra of AA, and denoted P​APA.

  2. 2.

    Pullback of a Schochet fibration along any ∗*-homomorphism is a Schochet fibration. Given a ∗*-homomorphism f:B→Cf:B\rightarrow C, denote by Z⁡(f)Z(f) the pullback B×CP​CB\times_{C}PC. Z⁡(f)Z(f) is called the mapping cylinder of ff, and the canonical map Z⁡(f)→BZ(f)\rightarrow B is a Schochet fibration (and a homotopy equivalence).

    Concretely, we have

    Z(f)={(b,γ)∣b∈B,γ∈PC,γ(0)=f(b)}.Z(f)=\{(b,\gamma)\mid b\in B,\gamma\in PC,\gamma(0)=f(b)\}.

    There is also a canonical map ev1:Z⁡(f)→C\operatorname{ev}_{1}:Z(f)\rightarrow C which is also a Schochet fibration. By definition, the mapping cone of ff fits in the short exact sequence

    0→C⁡(f)→Z⁡(f)→ev1C→0.0\rightarrow C(f)\rightarrow Z(f)\xrightarrow{\operatorname{ev}_{1}}C\rightarrow 0.

    This sequence is furthermore semi-split and is called the mapping cone sequence. It will be extremely important for us in Section 3.3.

    In the special case that ff is an inclusion, Z⁡(f)Z(f) is isomorphic to all paths in CC which start at BB.

  3. 3.

    The maximal tensor product with an auxilliary algebra of a Schochet fibrant cartesian square remains a Schochet fibrant cartesian square. The minimal tensor product with an auxilliary algebra of of a mapping cone sequence remains a mapping cone sequence.

The following proposition discusses properties of 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} and LhL_{h}.

Proposition 3.1.
  1. 1.

    The ∞\infty-category 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is locally small, and is canonically equivalent to the ∞\infty-category presented by the Kan-enriched1818 18 we implicitly always view a topologically enriched category as a Kan enriched category category 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, i.e., by taking its homotopy coherent nerve.

  2. 2.

    𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is pointed and LhL_{h} is reduced, i.e. maps the zero algebra to the zero object in 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}.

  3. 3.

    𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} has finite limits and countable coproducts. LhL_{h} preserves finite products and countable coproducts.

  4. 4.

    For every left-exact ∞\infty-category 𝒟\mathcal{D}, the equivalence in Equation 3.1 restricts to an equivalence

    𝐅𝐮𝐧lex​(𝖦𝖢∗​𝖠𝗅𝗀hsep,𝒟)→≃Lh∗𝐅𝐮𝐧h,S​c​h​(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}^{\operatorname{lex}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h}^{*}}\mathbf{Fun}^{h,Sch}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}),

    where the left-hand entity denotes the full subcategory of 𝐅𝐮𝐧⁡(𝖦𝖢∗​𝖠𝗅𝗀hsep,𝒟)\mathbf{Fun}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D}) spanned by left-exact functors.

  5. 5.

    Lh:𝖦𝖢∗​𝖠𝗅𝗀sep→𝖦𝖢∗​𝖠𝗅𝗀hsepL_{h}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} has a symmetric monoidal refinement for both the minimal and maximal tensor products on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. Moreover, the functors

    ⊗?:𝖦𝖢∗𝖠𝗅𝗀hsep×𝖦𝖢∗𝖠𝗅𝗀hsep→𝖦𝖢∗𝖠𝗅𝗀hsep\otimes_{?}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\times\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}

    are bi-left exact for ?∈{min,max}?\in\{\operatorname{min,max}\}.

  6. 6.

    For every left-exact and symmetric monoidal ∞\infty-category 𝒟\mathcal{D} and ?∈{min,max}?\in\{\min,\max\}, the pullback along the symmetric monoidal refinement of LhL_{h} induces an equivalence

    𝐅𝐮𝐧⊗?/laxlex(𝖦𝖢∗𝖠𝗅𝗀hsep,𝒟)→≃Lh∗𝐅𝐮𝐧⊗?/laxh,S​c​h(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}^{\operatorname{lex}}_{\otimes_{?}/\operatorname{lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h}^{*}}\mathbf{Fun}^{h,Sch}_{\otimes_{?}/\operatorname{lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}),

    where the subscript ⊗?/lax\otimes_{?}/\operatorname{lax} indicates two separate formulas, one for symmetric monoidal functors and the other for lax monoidal functors.

Proof.

The proofs of [17, Section 3] can be readily adapted to this situation. The Real structure poses no extra difficulty. Note that the key point for the left-exact assertions is that the category of separable GG-C∗C^{*}-algebras becomes a category of fibrant objects with fibrations as the Schochet fibrations and weak equivalences as the homotopy equivalences. ∎

Remark 3.1.

For later use, we explicitly mention an easy corollary of Section 3.1.4: we have an equivalence of functors

Lh∘(C0​(ℝ0,1,−))≃Ω∘Lh:𝖦𝖢∗​𝖠𝗅𝗀sep→𝖦𝖢∗​𝖠𝗅𝗀hsep.L_{h}\circ(C_{0}(\mathbb{R}^{0,1},-))\simeq\Omega\circ L_{h}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}.

The details are exactly the same as in [17, Example 3.19].

We also mention at this juncture that all the subsequent localizations leading to KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} will be left-exact Dwyer-Kan localizations. Hence we can take C0​(ℝ0,1,−)C_{0}(\mathbb{R}^{0,1},-) (descended to the category under consideration) as a model for the loops functor in each of the subsequent localizations.

We end this subsection by a casting the idea of the proof of Section 2.1 using the language of fiber sequences.

Proposition 3.1.

There exists a fiber sequence in 𝖦2​𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} of the form

𝒮→ev0ℂ→𝜄C​l0,1,\mathcal{S}\xrightarrow{\operatorname{ev}_{0}}\mathbb{C}\xrightarrow{\operatorname{\iota}}Cl^{0,1}, (3.2)

where ι\iota is the canonical inclusion of ℂ≅C​l0,0\mathbb{C}\cong Cl^{0,0} into C​l0,1Cl^{0,1}.

Proof.

This is immediate from Equation 2.1 and Section 3.1. ∎

3.2 Enforcing 𝒦G\mathcal{K}_{G}-stability

At the second step, we want to enforce a equivariant form of stability in 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}. The idea is to enforce that the map induced on the GG-C∗C^{*}-algebras of compact operators by isometric inclusions of GG-Hilbert spaces become equivalences. We begin with a couple of definitions.

Definition 3.2.
  • •

    A morphism f:A→Bf:A\rightarrow B in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is said to be a 𝒦G{\mathcal{K}_{G}}-equivalence if the induced map

    f⊗1𝒦G:A⊗𝒦G→B⊗𝒦Gf\otimes 1_{{\mathcal{K}_{G}}}:A\otimes{\mathcal{K}_{G}}\rightarrow B\otimes{\mathcal{K}_{G}}

    is a homotopy equivalence.

  • •

    For any ∞\infty-category 𝒟\mathcal{D}, a functor F:𝖦𝖢∗​𝖠𝗅𝗀sep→𝒟F:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathcal{D} is said to be GG-stable if for every isometric embedding of separable GG-Hilbert spaces V′↪VV^{\prime}\hookrightarrow V, with V′≠0V^{\prime}\neq 0, and for all objects A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the induced map F⁡(A⊗𝒦⁡(V))→F⁡(A⊗𝒦⁡(V′))F(A\otimes\mathcal{K}(V))\rightarrow F(A\otimes\mathcal{K}(V^{\prime})) is an equivalence.

Remark 3.2.

It is easy to see that a homotopy invariant functor on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} inverts 𝒦G{\mathcal{K}_{G}}-equivalences if and only if is GG-stable. See [47, Proposition 2.2] for a proof. It so turns out that inverting the 𝒦G\mathcal{K}_{G}-equivalences enables one to control the mapping spaces in the localization, whereas to verify that a homotopy invariant functor indeed inverts 𝒦G\mathcal{K}_{G}-equivalences, one usually just checks GG-stability.

We denote by 𝒲𝒦G\mathcal{W}_{{\mathcal{K}_{G}}} the (essentially small) class of 𝒦G\mathcal{K}_{G}-equivalences.

Definition 3.2.

Denote by S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} the Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} at Lh​(𝒲𝒦G)L_{h}(\mathcal{W}_{\mathcal{K}_{G}}), and denote by

L𝒦G:𝖦𝖢∗​𝖠𝗅𝗀hsep→S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsepL_{{\mathcal{K}_{G}}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}

the localization functor.

Note that this means that the canonical functor

Lh,𝒦G:𝖦𝖢∗​𝖠𝗅𝗀sep→Lh𝖦𝖢∗​𝖠𝗅𝗀hsep→L𝒦GS𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsepL_{h,{\mathcal{K}_{G}}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\xrightarrow{L_{h}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{{\mathcal{K}_{G}}}}\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}

is a Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} at 𝒲h∪𝒲𝒦G\mathcal{W}_{h}\cup\mathcal{W}_{{\mathcal{K}_{G}}}, whence we have an equivalence of functor categories

𝐅𝐮𝐧⁡(S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep,𝒟)→≃Lh,𝒦G∗𝐅𝐮𝐧h,𝒦G​(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}), (3.3)

where the right-hand side denotes the full subcategory of 𝐅𝐮𝐧⁡(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟)\mathbf{Fun}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}) spanned by functors which are homotopy invariant and GG-stable.

Proposition 3.3.
  1. 1.

    The ∞\infty-category S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is canonically equivalent to the full-subcategory of 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} spanned by 𝒦G{\mathcal{K}_{G}}-stable algebras. When GG is compact, the functor L𝒦GL_{{\mathcal{K}_{G}}} is in fact the left-adjoint of a left Bousfield localization.

  2. 2.

    S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} has finite limits and countable coproducts. Lh,𝒦GL_{h,{\mathcal{K}_{G}}} preserves finite products and countable coproducts. L𝒦GL_{\mathcal{K}_{G}} is left-exact.

  3. 3.

    For every left-exact ∞\infty-category 𝒟\mathcal{D}, the equivalence in Equation 3.3 restricts to an equivalence

    𝐅𝐮𝐧lex​(S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep,𝒟)→≃Lh,𝒦G∗𝐅𝐮𝐧h,𝒦G,S​c​h​(𝖦𝖢∗​𝖠𝗅𝗀sep,𝒟).\mathbf{Fun}^{\operatorname{lex}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},Sch}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}). (3.4)
  4. 4.

    Countable coproducts in S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} are given by countable direct sums of the respective C∗C^{*}-algebras. The canonical map from a binary (resp. countable) coproduct to a binary (resp. countable) product in S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is an equivalence, whence S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is a semi-additive ∞\infty-category.

  5. 5.

    For every left-exact semi-additive ∞\infty-category 𝒟\mathcal{D} with countable coproducts, the equivalence in Equation 3.4 restricts to an equivalence

    𝐅𝐮𝐧lex,∐ω(S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep,𝒟)→≃Lh,𝒦G∗𝐅𝐮𝐧h,𝒦G,Sch,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},Sch,\oplus_{\omega}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}), (3.5)

    where the superscripts ∐ω,⊕ω\coprod_{\omega},\oplus_{\omega} denote countable coproduct and countable sum preserving functors, respectively.

  6. 6.

    L𝒦G:𝖦𝖢∗​𝖠𝗅𝗀hsep→S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsepL_{\mathcal{K}_{G}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} has a symmetric monoidal refinement for both the tensor products on 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}. Consequently the same assertion is also true for Lh,𝒦GL_{h,{\mathcal{K}_{G}}}. Moreover, the functors

    ⊗?:S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep×S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep\otimes_{?}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\times\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}

    are bi-left exact and bi-countable coproduct preserving for ?∈{min,max}?\in\{\operatorname{min,max}\}.

  7. 7.

    For every symmetric monoidal left-exact semi-additive ∞\infty-category 𝒟\mathcal{D} with countable coproducts, the pullback along the symmetric monoidal refinement of Lh,𝒦GL_{h,{\mathcal{K}_{G}}} induces an equivalence

    𝐅𝐮𝐧⊗?/laxlex,∐ω(S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep,𝒟)→≃Lh,𝒦G∗𝐅𝐮𝐧⊗?/laxh,𝒦G,Sch,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟).\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega}}_{\otimes_{?}/\operatorname{lax}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},Sch,\oplus_{\omega}}_{\otimes_{?}/\operatorname{lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}).
Proof.

This follows by combining the approaches in [17, Section 4], [11, Remark 3.34] and [25, Lemma 3.18, Corollary 3.19]. The Real structure poses no extra difficulty. ∎

3.3 Enforcing !!-excision

Let

0{\lx@inpgf@ignorespaces 0}A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}C{\lx@inpgf@ignorespaces C}0{\lx@inpgf@ignorespaces 0}f\scriptstyle{\lx@inpgf@ignorespaces f}s\scriptstyle{\lx@inpgf@ignorespaces s}

be an extension of algebras in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, where the cpc-split ss exists if we are dealing with the case !=se!=\operatorname{se}. From this extension, we form the natural diagram

0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}A{\lx@inpgf@ignorespaces A}B{\lx@inpgf@ignorespaces B}C{\lx@inpgf@ignorespaces C}0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}C⁡(f){\lx@inpgf@ignorespaces{C(f)}}Z⁡(f){\lx@inpgf@ignorespaces{Z(f)}}C{\lx@inpgf@ignorespaces C}0{\lx@inpgf@ignorespaces 0}Q⁡(f){\lx@inpgf@ignorespaces{Q(f)}}0{\lx@inpgf@ignorespaces 0}ιf\scriptstyle{\lx@inpgf@ignorespaces\iota_{f}}f\scriptstyle{\lx@inpgf@ignorespaces f}hf\scriptstyle{\lx@inpgf@ignorespaces h_{f}}s\scriptstyle{\lx@inpgf@ignorespaces s}πf\scriptstyle{\lx@inpgf@ignorespaces\pi_{f}}f~\scriptstyle{\lx@inpgf@ignorespaces\tilde{f}}s~\scriptstyle{\lx@inpgf@ignorespaces\tilde{s}}s^\scriptstyle{\lx@inpgf@ignorespaces\hat{s}} (3.6)

We now explain the algebras and the morphisms in the above diagram. The middle row is the mapping cone extension of ff as described in Section 3.1.2. hfh_{f} is the map b↦(b,constf⁡(b))b\mapsto(b,\mathrm{const}_{f(b)}), and ιf\iota_{f} is the map a↦(a,0)a\mapsto(a,0) (without loss of generality, we are assuming that AA is an ideal in BB). πf:C⁡(f)→Q⁡(f)\pi_{f}:C(f)\rightarrow Q(f) is the cokernel of ιf\iota_{f}. Note that we have an isomorphism

Q(f)≅{(c,γ)∈C×PC∣γ(0)=c,γ(1)=0}≅C0([0,1),C),Q(f)\cong\{(c,\gamma)\in C\times PC\mid\gamma(0)=c,\gamma(1)=0\}\cong C_{0}([0,1),C),

and therefore Q⁡(f)Q(f) is contractible.

We now note that if ss is a cpc-split of ff, then it induces natural cpc-splits s~\tilde{s} and s^\hat{s} of f~\tilde{f} and πf\pi_{f}, given by s~​(c)=(s⁡(c),constc)\tilde{s}(c)=(s(c),\mathrm{const}_{c}) and s^​(c,γ)=(s⁡(c),γ)\hat{s}(c,\gamma)=(s(c),\gamma).

We denote by W!^\hat{W_{!}} the (essentially small) class of morphisms Lh,𝒦G​(ιf)L_{h,{\mathcal{K}_{G}}}(\iota_{f}) for all !!-exact sequences. We then define W!W_{!} to be the closure of W!^\hat{W_{!}} inside S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} under pullbacks, the 2-out-of-3 property and countable sums. Note that W!{W_{!}} is also essentially small.

Definition 3.6.

Denote by S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}} the Dwyer-Kan localization of S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} at W!W_{!}, and denote by

L!,⊕ω:S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sepL_{!,\oplus_{\omega}}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}

the localization functor.

Note that the composite

Lh,𝒦G,!,⊕ω:𝖦𝖢∗𝖠𝗅𝗀sep→Lh𝖦𝖢∗𝖠𝗅𝗀hsep→L𝒦GS𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→L!,⊕ωS𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sepL_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\xrightarrow{L_{h}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{\mathcal{K}_{G}}}\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{!,\oplus_{\omega}}}\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}

is a Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, as can be seen from the proof of [11, Proposition 3.40]. Before describing the key properties of this localization, we mention the motivation for closing W^!\hat{W}_{!} under countable sums.

Remark 3.6.

It is a non-trivial property of classical K​KKK- and EE-categories for separable C∗C^{*}-algebras that they have countable coproducts, which are furthermore modeled by countable direct sums of the respective C∗C^{*}-algebras. If we do not close up W^!\hat{W}_{!} under countable sums, then there is no formal reason why our to-be-constructed KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} category will have countable coproducts (see the next paragraph too). The issue therefore arises when we want to extend KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} to the large category KKG!,∞\mathrm{KK}^{G}_{!,\infty} on all of 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}: on the one hand, we can simply consider Indℵ0\operatorname{Ind}_{\aleph_{0}}-completion of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}, but then we would destroy the countable coproducts which already exist in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} (since a posteori the homotopy category of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is equivalent to the classical bivariant KK-categories), and would therefore be an unnatural object to consider. On the other hand, our current approach (as done in Section 3.7) of taking Indℵ1(KK!,∞G,sep)\operatorname{Ind}_{\aleph_{1}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}) would a priori have no reason to have countable coproducts, but would have all uncountable filtered colimits, and would be yet another unnatural object! Of course, if we already know the comparison between the homotopy category of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} and the classical bivariant KK-categories, then the Indℵ1\operatorname{Ind}_{\aleph_{1}}-completion of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} works out fine and becomes a presentable stable ∞\infty-category, but we want to postpone this comparison until the very end. Thus, it calls for enforcing that our KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} categories have countable coproducts.

Having said that, we mention that the step of closing up W^!\hat{W}_{!} under countable sums is only relevant for non-separable algebras (and even then, more for the aesthetic features of our large categories). In particular, if the reader is only interested in separable C∗C^{*}-algebras, then this step can be omitted, and one would still get a stable ∞\infty-categorical refinement of the classical bivariant KK-categories for separable C∗C^{*}-algebras which would a fortiori have countable coproducts.

Proposition 3.6.
  1. 1.

    The ∞\infty-category S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}} is left-exact, semi-additive and posseses countable coproducts.

  2. 2.

    The localization functor L!,⊕ωL_{!,\oplus_{\omega}} is left-exact and countable sum preserving. The functor Lh,𝒦G,!L_{h,{\mathcal{K}_{G}},!} is !!-exact.

  3. 3.

    For every left-exact semi-additive ∞\infty-category 𝒟\mathcal{D} admitting countable coproducts, we have equivalences

    𝐅𝐮𝐧lex,∐ω(S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep,𝒟)→≃L!,⊕∗𝐅𝐮𝐧lex,∐ω,W^!(S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep,𝒟)→≃Lh,𝒦G∗𝐅𝐮𝐧h,𝒦G,!+Sch,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟),\displaystyle\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{!,\oplus}^{*}}\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega},\hat{W}_{!}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}}}^{*}}\mathbf{Fun}^{{h,{\mathcal{K}_{G}},!+Sch,\oplus}_{\omega}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}),

    (3.7)

    where the superscript W^!\hat{W}_{!} in the middle entity stands for functors on S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} which map morphisms in W^!\hat{W}_{!} to equivalences, and the superscript !! in the last entity stands for functors on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} which map !!-exact sequences to fiber sequences.

  4. 4.

    When !=se!=\operatorname{se},

    Lse,⊕ω:S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,se,⊕ωsepL_{\operatorname{se},\oplus_{\omega}}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,\mathrm{se},\oplus_{\omega}}^{\mathrm{sep}}

    has a symmetric monoidal refinement for both the tensor products on S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}. When !=ex!=\operatorname{ex},

    Lex,⊕ω:S𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,ex,⊕ωsepL_{\operatorname{ex},\oplus_{\omega}}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,\mathrm{ex},\oplus_{\omega}}^{\mathrm{sep}}

    has a symmetric monoidal refinement for only the maximal tensor product on S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}. Consequently, the same assertions are true for Lh,𝒦G,se,⊕ωL_{h,{\mathcal{K}_{G}},\operatorname{se},\oplus_{\omega}} and Lh,𝒦G,ex,⊕ωL_{h,{\mathcal{K}_{G}},\operatorname{ex},\oplus_{\omega}}.

    Moreover, the functors

    ⊗?:S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep×S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\otimes_{?}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}\times\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}

    are bi-left exact and bi-countable coproduct preserving (for every choice of (?,!)(?,!) except (min,ex)(\operatorname{min,ex})).

  5. 5.

    For every symmetric monoidal left-exact semi-additive ∞\infty-category 𝒟\mathcal{D} admitting countable coproducts, the pullback along the symmetric monoidal refinement of Lh,𝒦G,!,⊕ωL_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}} (as discussed in the previous assertion) induces an equivalence

    𝐅𝐮𝐧⊗?/laxlex,∐ω(S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep,𝒟)→≃Lh,𝒦G,!,⊕ω∗𝐅𝐮𝐧⊗?/laxh,𝒦G,!+Sch,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟).\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega}}_{\otimes_{?}/\operatorname{lax}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}^{*}}\mathbf{Fun}^{{h,{\mathcal{K}_{G}},!+Sch,\oplus_{\omega}}}_{\otimes_{?}/\operatorname{lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}). (3.8)
Proof.

This follows by combining the approaches in [17, Section 5] and [11, Remark 3.35]. Note that closing up W^!\hat{W}_{!} under countable sums has only been considered in [11], and an argument for the localization L!,⊕ωL_{!,\oplus_{\omega}} to be countable coproduct preserving is omitted in loc.​ cit.​ This however follows from a dual version of [49, Theorem 2.6.4]1919 19 note that loc.​ cit.​ is written with cofibration categories, whereas our current business is with fibration categories. However, loc.​ cit.​ uses [18, Proposition 7.7.1] in the proof, which is indeed written with fibration categories.. ∎

We end this subsection with an important lemma, which will be useful in formulating the universal property of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} in the next section. The lemma can be considered as an automatic Schochet-exactness result, which is ubiquitous for applications since Schochet exactness of a functor can be very difficult to verify.

Lemma 3.8.

Any homotopy invaraint and !!-exact functor from 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to a stable ∞\infty-category is automatically Schochet exact.

Proof.

The proof can be taken directly from [17, Lemma 5.2]. ∎

3.4 Inverting Bott

This subsection is going to somewhat different than the corresponding step in the complex theory as developed in [17, Sections 6,7]. Indeed, in the complex case, an analysis of the Toeplitz extensions

0→𝒦⁡(l2​ℕ)⊗B→𝒯0⊗B→C0​(ℝ)⊗B→00\rightarrow\mathcal{K}(l^{2}\mathbb{N})\otimes B\rightarrow\mathcal{T}_{0}\otimes B\rightarrow C_{0}(\mathbb{R})\otimes B\rightarrow 0
2020 20 That the Toeplitz algebra is nuclear can be deduced from nuclear C∗C^{*}-algebras being closed under extensions, see [7, Section IV.3.1] for details.

yields a boundary map

C0​(ℝ2)⊗B→β!,BBC_{0}(\mathbb{R}^{2})\otimes B\xrightarrow{\beta_{!,B}}B

in (the complex analog of) S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}, which subsequently are inverted yielding the stable ∞\infty-category KKG,sep!,∞,ℂ\mathrm{KK}^{G,\mathrm{sep}}_{!,\infty,\mathbb{C}} (check loc.​ cit.​ for details). This also shows that Ω\Omega is a self-inverse endofunctor on KKG,sep!,∞,ℂ\mathrm{KK}^{G,\mathrm{sep}}_{!,\infty,\mathbb{C}}.

In the Real case, one has to work with the Real version of the Toeplitz extension. We discuss it next. Before proceeding, we setup some notation.

Notation 3.8.

Let ℝp,q\mathbb{R}^{p,q} denote the Real space ℝp+q\mathbb{R}^{p+q}, with the involution κp,q\kappa_{p,q} given by

κp,q​(x1,x2,…,xp+q)=(−x1,−x2,…,−xp,xp+1,xp+2,…,xp+q).\kappa_{p,q}(x_{1},x_{2},...,x_{p+q})=(-x_{1},-x_{2},...,-x_{p},x_{p+1},x_{p+2},...,x_{p+q}).

Denote by 𝕊p,q\mathbb{S}^{p,q} the unit sphere in ℝp,q\mathbb{R}^{p,q} with the induced involution.

The following result is going to be our workhorse for the Real Bott periodicity.

Proposition 3.8.

There exists a semi-split extension of Real C∗C^{*}-algebras

0→𝒦⁡(l2​ℕ)→𝒯R→C⁡(𝕊1,1),0\rightarrow\mathcal{K}(l^{2}\mathbb{N})\rightarrow\mathcal{T}^{R}\rightarrow C(\mathbb{S}^{1,1}),

where 𝒯R\mathcal{T}^{R} is the Real isometry classfier C∗C^{*}-algebra, i.e., there is a distinguised Real isometry vv in 𝒯R\mathcal{T}^{R} such that for any unital (non-equivariant) Real C∗C^{*}-algebra AA, there is a bijection of sets

Homu⁡(𝒯R,A)→≅Isom⁡(A),φ↦φ⁡(v){\operatorname{Hom}}_{u}(\mathcal{T}^{R},A)\xrightarrow{\cong}\operatorname{Isom}(A),\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \varphi\mapsto\varphi(v)

between the set of unital, Real homomorphisms from 𝒯R\mathcal{T}^{R} to AA and the set of Real isometries in AA.

Before proving the above result, we begin with a quick justification that 𝒯R\mathcal{T}^{R} indeed exists, and also set up some notation along the way.

Lemma 3.8.

The Real C∗C^{*}-algebra 𝒯R\mathcal{T}^{R} as defined in Section 3.4 exists.

Proof.

Recall that the complex Toeplitz algebra 𝒯ℂ\mathcal{T^{\mathbb{C}}}, given by the C∗C^{*}-subalgebra generated by the unilateral shift (denoted 𝜾\boldsymbol{\iota} from now on) in ℬ​(l2​(ℕ))\mathcal{B}(l^{2}(\mathbb{N})), is the universal (complex) isometry classifier ([19]). It therefore follows that one model for 𝒯R\mathcal{T}^{R} is 𝒯ℂ\mathcal{T}^{\mathbb{C}} equipped with the unique Real structure such that the unilateral shift is fixed by it. It is also easily seen to be the same as the Real C∗C^{*}-subalgebra of ℬ​(l2​(ℕ))\mathcal{B}(l^{2}(\mathbb{N})) generated by the unilateral shift, where the Real structure on the Hilbert space l2​(ℕ)l^{2}(\mathbb{N}) is by complex conjugation (as always). ∎

We now show that C⁡(𝕊1,1)C(\mathbb{S}^{1,1}) is also a universal Real C∗C^{*}-algebra.

Lemma 3.8.

C⁡(𝕊1,1)C(\mathbb{S}^{1,1}) is the Real unitary classifier C∗C^{*}-algebra.

Proof.

Again as before, the complex version of this result is well-known, see for example [56, Proposition 2.3.4]. It follows that the Real structure on the C∗C^{*}-algebra of continuous functions on the circle should be so defined that the identity function on the circle is a Real unitary. Since the Real structure on the codomain ℂ\mathbb{C} is complex conjugation, it directly follows from the definitions that the Real structure stemming from the Real space 𝕊1,1\mathbb{S}^{1,1} is indeed the right one. ∎

Proof (of Section 3.4).

The morphism 𝒯R→C⁡(𝕊1,1)\mathcal{T}^{R}\xrightarrow{}C(\mathbb{S}^{1,1}) is given by mapping 𝜾\boldsymbol{\iota} (in the concrete model of 𝒯R\mathcal{T}^{R} mentioned in Section 3.4) to the inclusion 𝕊1,1↪ℂ\mathbb{S}^{1,1}\hookrightarrow\mathbb{C}. The kernel of φ\varphi contains

𝜾n​(1l2​ℕ−𝜾​𝜾∗)​𝜾∗m​∀n,m≥0,\boldsymbol{\iota}^{n}(1_{l^{2}\mathbb{N}}-\boldsymbol{\iota}\boldsymbol{\iota}^{*}){\boldsymbol{\iota}^{*}}^{m}\penalty\ \forall\penalty\ n,m\geq 0,

and therefore also contains the Real C∗C^{*}-subalgebra 𝒦⁡(l2​ℕ)\mathcal{K}(l^{2}\mathbb{N}) of ℬ​(l2​(ℕ))\mathcal{B}(l^{2}(\mathbb{N})). It is well-known that upon forgetting the Real structure, the kernel of φ\varphi is precisely 𝒦⁡(l2​ℕ)\mathcal{K}(l^{2}\mathbb{N}), see for example [56, Section 2.4]. This shows the existence of the extension.

To show that it also admits a Real cpc-split, one directly checks that the cpc-split described in [17, Remark 6.7] is a Real map. ∎

Corollary 3.8.

There exists a semi-split extension of Real C∗C^{*}-algebras

0→𝒦⁡(l2​ℕ)→𝒯0R→C0​(ℝ1,0)→0.0\rightarrow\mathcal{K}(l^{2}\mathbb{N})\rightarrow\mathcal{T}^{R}_{0}\rightarrow C_{0}(\mathbb{R}^{1,0})\rightarrow 0. (3.9)

Given A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and a homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, split exact functor F:𝖦𝖢∗​𝖠𝗅𝗀sep→𝒟F:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathcal{D} taking values in the group objects of a semi-additive ∞\infty-category 𝒟\mathcal{D}, F⁡(A⊗𝒯0R)≃0F(A\otimes\mathcal{T}^{R}_{0})\simeq 0.

Proof.

The existence of the semi-split extension readily follows from Section 3.4 and the isomorphism of Real C∗C^{*}-algebras

C0​(ℝ1,0)≅ker⁡(C⁡(𝕊1,1)→ev(0,1)ℂ).C_{0}(\mathbb{R}^{1,0})\cong\ker(C(\mathbb{S}^{1,1})\xrightarrow{\operatorname{ev}_{(0,1)}}\mathbb{C}).

The second part of the corollary is proven just as in the complex case, see [17, Section 6] and [53, Corollary 1.5.3]. ∎

Having Section 3.4 at our disposal, we can again emulate the treatment of [17] without the Real structure posing any extra difficulty.

For each B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, Equation 3.9 yields a semi-split extension

0→𝒦⁡(l2​ℕ)⊗B→𝒯0R⊗B→C0​(ℝ1,0)⊗B→0.0\rightarrow\mathcal{K}(l^{2}\mathbb{N})\otimes B\rightarrow\mathcal{T}_{0}^{R}\otimes B\rightarrow C_{0}(\mathbb{R}^{1,0})\otimes B\rightarrow 0.

Applying the semi-split exact functor Lh,𝒦G,!,⊕ωL_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}} to these extensions, one obtains a Puppe sequence

⋯→Lh,𝒦G,!,⊕ω(C0(ℝ1,1)⊗B)→β!,BLh,𝒦G,!,⊕ω(𝒦(l2ℕ)⊗B)→Lh,𝒦G,!,⊕ω(𝒯0R⊗B)→Lh,𝒦G,!,⊕ω(C0(ℝ1,0)⊗B)\displaystyle\cdots\rightarrow L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}\!\bigl(C_{0}(\mathbb{R}^{1,1})\otimes B\bigr)\xrightarrow{\beta_{!,B}}L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}\!\bigl(\mathcal{K}(l^{2}\mathbb{N})\otimes B\bigr)\rightarrow L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}\!\bigl(\mathcal{T}_{0}^{R}\otimes B\bigr)\rightarrow L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}\!\bigl(C_{0}(\mathbb{R}^{1,0})\otimes B\bigr)

(3.10)

where β!,B\beta_{!,B} are the relevant “boundary maps” in S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}. Using the stability of S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}, we obtain a natural transformation

β!:=β!,ℂ⊗−:C0(ℝ1,1)⊗−⟹idS𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep:S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep→S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep.\beta_{!}:=\beta_{!,\mathbb{C}}\otimes-:C_{0}(\mathbb{R}^{1,1})\otimes-\implies\operatorname{id}_{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}.

The important feature of this natural transformation is the following.

Corollary 3.10.

If AA is a group object in S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}, then the component of β!\beta_{!}

β!,A:C0(ℝ1,1)⊗!A→A\beta_{!,A}:C_{0}(\mathbb{R}^{1,1})\otimes_{!}A\rightarrow A

is an equivalence.

Proof.

The proof of [17, Corollary 6.11] will work with the obvious modifications. ∎

We are now in a position to define the small stable ∞\infty-category KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}. We denote by WBottW_{\operatorname{Bott}} the (essentially small) class of maps β!,B\beta_{!,B} as in Equation 3.10.

Definition 3.10.

Define KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} to be the Dwyer-Kan localization of S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}} at WBottW_{\operatorname{Bott}}, and denote by

LBott:S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep→KK!,∞G,sepL_{\operatorname{Bott}}:\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}

the localization functor.

Note that the composite

kk!,∞G,sep:𝖦𝖢∗𝖠𝗅𝗀sep→Lh𝖦𝖢∗𝖠𝗅𝗀hsep→L𝒦GS𝒦G𝖦𝖢∗𝖠𝗅𝗀hsep→L!,⊕ωS𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep→LBottKK!,∞G,sep\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\xrightarrow{L_{h}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{\mathcal{K}_{G}}}\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{!,\oplus_{\omega}}}\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}\xrightarrow{L_{\operatorname{Bott}}}\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} (3.11)

is a Dwyer-Kan localization of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, as can be deduced from the proof of [11, Proposition 3.40].

Proposition 3.11.
  1. 1.

    KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is left-exact. LBottL_{\operatorname{Bott}} is also left-exact and has a fully faithful left-adjoint. KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} can be realized as the full subcategory of group objects of S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}.

  2. 2.

    KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is a small stable ∞\infty-category.

  3. 3.

    KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is countably cocomplete. For a countable collection (Bn)n∈ℕ(B_{n})_{n\in\mathbb{N}} of algebras in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we have an equivalence

    ∐n∈ℕkk!,∞G,sep(Bn)→≃kk!,∞G,sep(⊕n∈ℕBn).\coprod_{n\in\mathbb{N}}\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}(B_{n})\xrightarrow{\simeq}\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}(\oplus_{n\in\mathbb{N}}B_{n}).

    When !=ex!=\operatorname{ex}, kk!,∞G,sep\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}} even preserves general countable filtered colimits.

  4. 4.

    Every left-exact functor from S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}} to a left-exact additive ∞\infty-category 𝒟\mathcal{D} automatically factors (essentially uniquely) through KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}. More precisely, for every left-exact ∞\infty-category 𝒟\mathcal{D}, we have an equivalence

    𝐅𝐮𝐧lex(KK!,∞G,sep,𝒟)→≃LBott∗𝐅𝐮𝐧lex(S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep,𝒟).\mathbf{Fun}^{\operatorname{lex}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{\operatorname{Bott}}^{*}}\mathbf{Fun}^{\operatorname{lex}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}},\mathcal{D}).
  5. 5.

    For every countably cocomplete stable ∞\infty-category 𝒟\mathcal{D}, we have an equivalence

    𝐅𝐮𝐧colimω(KK!,∞G,sep,𝒟)→≃kk!,∞G,sep∗𝐅𝐮𝐧h,𝒦G,!,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}^{\operatorname{colim}_{\omega}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{{\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}),

    where the superscript colimω\operatorname{colim}_{\omega} denotes the full subcategory of functors which are countable colimit preserving.

  6. 6.

    KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} has a symmetric monoidal refinement for both the tensor products when !=se!=\operatorname{se}, and only for the maximal tensor product when !=ex!=\operatorname{ex}.

  7. 7.

    LBottL_{\operatorname{Bott}} has a symmetric monoidal refinement for the tensor product(s) on S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}. Consequently, the same assertions are true for kk!,∞G,sep\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}. Moreover, the functors

    ⊗?:KK!,∞G,sep×KK!,∞G,sep→KK!,∞G,sep\otimes_{?}:\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}\times\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}\rightarrow\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}

    are bi-countable colimit preserving (for every choice of (?,!)(?,!) except (min,ex)(\operatorname{min,ex})).

  8. 8.

    For every left-exact symmetric monoidal additive ∞\infty-category 𝒟\mathcal{D}, pullback along the symmetric monoidal refinement(s) of LBottL_{\operatorname{Bott}} induces an equivalence

    𝐅𝐮𝐧⊗?/laxlex(KK!,∞G,sep,𝒟)→≃LBott∗𝐅𝐮𝐧⊗?/laxlex(S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep,𝒟).\mathbf{Fun}^{\operatorname{lex}}_{\otimes_{?}/\operatorname{lax}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{\operatorname{Bott}}^{*}}\mathbf{Fun}^{\operatorname{lex}}_{\operatorname{\otimes_{?}/\operatorname{lax}}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}},\mathcal{D}).
  9. 9.

    For every symmetric monoidal countably cocomplete stable ∞\infty-category 𝒟\mathcal{D}, pullback along the symmetric monoidal refinement(s) of kk!,∞G,sep\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}} induces an equivalence

    𝐅𝐮𝐧⊗?/laxcolimω(KK!,∞G,sep,𝒟)→≃kk!,∞G,sep∗𝐅𝐮𝐧⊗?/laxh,𝒦G,!,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟).\mathbf{Fun}^{\operatorname{colim}_{\omega}}_{\otimes_{?}/\operatorname{lax}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{{\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}_{\otimes_{?}/\operatorname{lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}).
Proof.

We give some details in this proof as the result is ubiquitous for what we do later.

Assertion 11 follows directly from Equation 3.9 and the dual version of [43, Proposition 5.2.7.4], as has been spelled out at the beginning of Section 7 in [17].

We now show Assertion 2. In light of [44, Proposition 1.4.2.27], it suffices to show KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is small, pointed, left-exact and the loop functor on it is an equivalence. The first three properties are clear in light of Assertion 1 and the work done in the previous three subsections. It remains to see that loops is an equivalence. But this follows from Section 3.4 and the last part of Assertion 1.

We now move onto Assertion 3. By Section 3.3.1, S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}} has countable coproducts, whence so does KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} being a Bousfield localization of it (see [45, Subsection 7.1.4]). Any stable ∞\infty-category having countable coproducts is automatically countably cocomplete. That countable coproducts in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} are modeled by countable direct sum of the algebras follows from Section 3.3.3 and because of general properties of (co)limits in a Bousfield localization; see again [45, Subsection 7.1.4]. The case of !=ex!=\operatorname{ex} is the content of [11, Proposition 3.17] (the Real structure poses no additional difficulty).

Assertion 4 follows directly from Section 3.4 and Section 3.4.

Assertion 5 is arguably the most important result from this section for us. It follows from the series of equivalences

𝐅𝐮𝐧colimω(KK!,∞G,sep,𝒟)→≃LBott∗𝐅𝐮𝐧lex,∐ω(S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep,𝒟)→≃Lh,𝒦G,!,⊕ω∗𝐅𝐮𝐧h,𝒦G,!+Sch,⊕ω(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟),\mathbf{Fun}^{\operatorname{colim}_{\omega}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{\operatorname{Bott}}^{*}}\mathbf{Fun}^{\operatorname{lex},\coprod_{\omega}}(\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}},\mathcal{D})\xrightarrow[\simeq]{L_{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}^{*}}\mathbf{Fun}^{{h,{\mathcal{K}_{G}},!+Sch,\oplus_{\omega}}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D}),

where the first equivalence follows from Assertion 4 and (the proof of) Assertion 3, and the second one is Equation 3.7. We now conclude using Section 3.3.

Assertion 6 follows from [35, Proposition 3.3.2] and the basic permeance properties of !!-exact sequences with respect to the minimal and maximal tensor products.

The first two parts of Assertion 7 follow immediately from the nuclearity of 𝒦⁡(l2​ℕ),𝒯R,C⁡(𝕊1,1)\mathcal{K}(l^{2}\mathbb{N}),\mathcal{T}^{R},C(\mathbb{S}^{1,1}) and [35, Proposition 3.3.2]. For the final part, we use the fact that a left-exact and countable coproduct preserving functor between stable ∞\infty-categories is automatically countable colimit preserving.

For Assertion 8, we build the diagram

𝐅𝐮𝐧⊗?/laxlex(KK!,sepG,∞,𝒟){\lx@inpgf@ignorespaces{\mathbf{Fun}_{\otimes_{?}/\operatorname{lax}}^{\operatorname{lex}}(KK_{!,\operatorname{sep}}^{G,\infty},\mathcal{D})}}𝐅𝐮𝐧⊗?/laxlex(S𝒦GG-C∗−algR,h,!,⊕ωsep,𝒟){\lx@inpgf@ignorespaces{\mathbf{Fun}_{\otimes_{?}/\operatorname{lax}}^{\operatorname{lex}}(S_{\mathcal{K}_{G}}G\operatorname{\!-\!}C^{*}\operatorname{\!-alg}_{\operatorname{R,h,!,\oplus}_{\omega}}^{\operatorname{sep}},\mathcal{D})}}𝐅𝐮𝐧⊗?/lax(KK!,sepG,∞,𝒟){\lx@inpgf@ignorespaces{\mathbf{Fun}_{\otimes_{?}/\operatorname{lax}}^{\operatorname{}}(KK_{!,\operatorname{sep}}^{G,\infty},\mathcal{D})}}𝐅𝐮𝐧⊗?/laxWBott(S𝒦GG-C∗−algR,h,!,⊕ωsep,𝒟){\lx@inpgf@ignorespaces{\mathbf{Fun}^{W_{\operatorname{Bott}}}_{\otimes_{?}/\operatorname{lax}}(S_{\mathcal{K}_{G}}G\operatorname{\!-\!}C^{*}\operatorname{\!-alg}_{\operatorname{R,h,!,\oplus_{\omega}}}^{\operatorname{sep}},\mathcal{D})}}LBott∗\scriptstyle{\lx@inpgf@ignorespaces L_{\operatorname{Bott}}^{*}}LBott∗,≃\scriptstyle{\lx@inpgf@ignorespaces L_{\operatorname{Bott}}^{*},\simeq}

The lower horizontal arrow is an equivalence from Section 3.4 and [35, Proposition 3.3.2]. The dashed arrow can be seen to exist using the fact that LBottL_{\operatorname{Bott}} is left-exact. It remains to show that it is an equivalence. For that, we use the following general fact about symmetric monoidal left-exact Dwyer-Kan localizations: for any symmetric monoidal ∞\infty-category 𝒞\mathcal{C} and an (essentially small) collection of morphisms W⊆𝒞W\subseteq\mathcal{C} which are a tensor ideal in 𝒞\mathcal{C}, if the Dwyer-Kan localization of 𝒞\mathcal{C} at WW is left-exact, then we have an equivalence

𝐅𝐮𝐧⊗?/laxlex(𝒞[W−1],ℰ)→≃LW∗𝐅𝐮𝐧⊗?/laxlex,W(𝒞,ℰ)\mathbf{Fun}^{\operatorname{lex}}_{\otimes_{?}/\operatorname{lax}}(\mathcal{C}[W^{-1}],\mathcal{E})\xrightarrow[\simeq]{L_{W}^{*}}\mathbf{Fun}^{\operatorname{lex},W}_{\otimes_{?}/\operatorname{lax}}(\mathcal{C},\mathcal{E})

for every left-exact symmetric monoidal ∞\infty-category ℰ\mathcal{E}. See [18, Proposition 7.5.6] for details.

The proof of Assertion 9 follows in parallel to the proof of Assertion 5, in light of Assertion 8. ∎

We end this subsection by mentioning a couple of important corollaries to the construction of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}.

Corollary 3.11.
  1. 1.

    In KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}, we have an equivalence q​A→≃AqA\xrightarrow{\simeq}A for all A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

  2. 2.

    The fiber sequence

    𝒮→ev0ℂ→𝜄C​l0,1\mathcal{S}\xrightarrow{\operatorname{ev}_{0}}\mathbb{C}\xrightarrow{\iota}Cl^{0,1}

    in 𝖦2​𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} as discussed in Section 3.1 remains a fiber sequence in KK!,∞G2,sep\mathrm{KK}_{!,\infty}^{G_{2},\mathrm{sep}}.

  3. 3.

    The composite

    (𝒮​⊗^​C​l0,1)u→ev0∗C​lu0,1→π1ℂ(\mathcal{S}\hat{\otimes}Cl^{0,1})_{u}\xrightarrow{{\operatorname{ev}_{0}}_{*}}Cl^{0,1}_{u}\xrightarrow{\pi_{1}}\mathbb{C}

    is an equivalence in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}.

Proof.

Assertion 1 is the content of [17, Lemma 11.4], the generalization to the equivariant case is routine. Assertion 2 follows directly from Section 3.1, since we have shown before that each of the localizations in Equation 3.11 after LhL_{h} are left-exact. Assertion 3 follows from Assertion 1 in light of the function algebra model of q​ℂq\mathbb{C} as described in Section 2.1.4. ∎

Remark 3.11.

We present a more direct proof of Section 3.4.3 in this remark. Consider the ladder of semi-split exact sequences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}

0{\lx@inpgf@ignorespaces 0}{f∈C0​((0,1],M2​(ℂ))∣f⁡(1)​dia}{\lx@inpgf@ignorespaces{\{f\in C_{0}((0,1],M_{2}(\mathbb{C}))\mid f(1)\penalty\ \text{dia}\}}}{f∈C⁡([0,1],M2​(ℂ))∣f⁡(0)=(∗000)&f⁡(1)​dia}{\lx@inpgf@ignorespaces\begin{array}[]{c}\{f\in C([0,1],M_{2}(\mathbb{C}))\mid f(0)=\begin{pmatrix}*&&0\\ 0&&0\end{pmatrix}\penalty\ \&\penalty\ f(1)\text{dia}\}\end{array}}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}ℂ⊕ℂ{\lx@inpgf@ignorespaces{\mathbb{C}\oplus\mathbb{C}}}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}0{\lx@inpgf@ignorespaces 0}inc\scriptstyle{\lx@inpgf@ignorespaces\operatorname{inc}}(ev1)(1,1)\scriptstyle{\lx@inpgf@ignorespaces(\operatorname{ev}_{1})_{(1,1)}}(ev0)(1,1)\scriptstyle{\lx@inpgf@ignorespaces(\operatorname{ev}_{0})_{(1,1)}}(ev0)(1,1)⊕(ev1)(1,1)\scriptstyle{\lx@inpgf@ignorespaces(\operatorname{ev}_{0})_{(1,1)}\oplus(\operatorname{ev}_{1})_{(1,1)}}id\scriptstyle{\lx@inpgf@ignorespaces\operatorname{id}}ι2\scriptstyle{\lx@inpgf@ignorespaces\iota_{2}}π1\scriptstyle{\lx@inpgf@ignorespaces\pi_{1}}

We have to show that the left vertical arrow is an equivalence in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}. This will follow once the other two vertical arrows are shown to be equivalences in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}. Only the case of the middle vertical arrow needs an argument. The fiber of

{f∈C⁡([0,1],M2​(ℂ))∣f⁡(0)=(∗000)&f⁡(1)​dia}→(ev0)1,1⊕(ev1)1,1ℂ⊕ℂ\{f\in C([0,1],M_{2}(\mathbb{C}))\mid f(0)=\begin{pmatrix}*&0\\ 0&0\end{pmatrix}\penalty\ \&\penalty\ f(1)\penalty\ \text{dia}\}\xrightarrow{(\operatorname{ev}_{0})_{1,1}\oplus(\operatorname{ev}_{1})_{1,1}}\mathbb{C}\oplus\mathbb{C}

is readily seen to be the mapping cone of the right lower corner inclusion ℂ→M2​(ℂ)\mathbb{C}\rightarrow M_{2}(\mathbb{C}), and hence is contractible in S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}.

We end this subsection by mentioning a 11-categorical universal property of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}. The nature of this universal property is different in flavor than the ones described earlier in this section, and is only needed so as to make the comparison with classical K​KKK- and EE-theory possible later. This technical result can be skipped until the reader reaches Section 6.

We need a definition before proceeding. See also [17, Section 13] for some definitions circling half exact additive 11-categories.

Definition 3.11.

Denote by WKK!,∞G,sepW_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}} the collection of morphisms inverted by the functor

kk!,∞G,sep:𝖦𝖢∗𝖠𝗅𝗀sep→KK!,∞G,sep.\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}.
Proposition 3.11.

(cf. [17, Proposition 13.13]) Let 𝒟\mathcal{D} be a half exact additive 11-category with countable coproducts. Let F:𝖦𝖢∗​𝖠𝗅𝗀sep→𝒟F:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathcal{D} be a functor which is homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, half exact with respect to !!-exact sequences, takes countable direct sums in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to countable coproducts in 𝒟\mathcal{D}, and suspension stable (i.e. for every morphism f:A→B∈𝖦𝖢∗​𝖠𝗅𝗀sepf:A\rightarrow B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, F⁡(f)F(f) is an isomorphism if and only if F⁡(Ω⁡(f))F(\Omega(f)) is an isomorphism). Then FF inverts WKK!,∞G,sepW_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}.

Proof.

Since KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} by construction is a series of Dwyer-Kan localizations of 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we need to show that we can construct factorizations as indicated by the dashed arrows below

𝖦𝖢∗​𝖠𝗅𝗀sep{\lx@inpgf@ignorespaces\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}}S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep{\lx@inpgf@ignorespaces\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}𝒟{\lx@inpgf@ignorespaces\mathcal{D}}S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep{\lx@inpgf@ignorespaces\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}}KK!,∞G,sep{\lx@inpgf@ignorespaces\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}Lh,𝒦G\scriptstyle{\lx@inpgf@ignorespaces L_{h,{\mathcal{K}_{G}}}}F\scriptstyle{\lx@inpgf@ignorespaces F}F′\scriptstyle{\lx@inpgf@ignorespaces F^{\prime}}L!,⊕ω\scriptstyle{\lx@inpgf@ignorespaces L_{!,\oplus_{\omega}}}F′′\scriptstyle{\lx@inpgf@ignorespaces F^{\prime\prime}}LBott\scriptstyle{\lx@inpgf@ignorespaces L_{\mathrm{Bott}}}F′′′\scriptstyle{\lx@inpgf@ignorespaces F^{\prime\prime\prime}} (3.12)

The first two hypothesis on FF yields the functor F′F^{\prime}. Note that F′F^{\prime} inverts W^!\hat{W}_{!}, as follows from [8, Theorem 21.4.4] (which states that FF yields natural long exact sequences) and a standard 5-lemma argument applied to Equation 3.6.

We now claim that F′F^{\prime} also inverts the closure W!W_{!} of W^!\hat{W}_{!} under 2-out-of-3, pullbacks, and countable sums. It suffices to show that the collection of morphisms inverted by F′F^{\prime} is closed under pullbacks and countable sums. The argument for pullbacks can be extracted verbatim from the proof of the analogous assertion in [17, Proposition 13.13]. That the collection of morphisms inverted by F′F^{\prime} are preserved under countable sums follows immediately from our hypothesis that the natural map

∐n∈ℕF(An)→F(⊕n∈ℕAn)\coprod_{n\in\mathbb{N}}F(A_{n})\xrightarrow{}F(\oplus_{n\in\mathbb{N}}A_{n})

is an isomorphism. Thus, we deduce the existence of F′′F^{\prime\prime}.

The argument for F′′F^{\prime\prime} inverting the maps β!,B\beta_{!,B} can be read off from the analogous step in the proof of [17, Proposition 13.13] (with the obvious changes to the Toeplitz extension in the Real case as discussed in Subsection 3.4). This shows the existence of F′′′F^{\prime\prime\prime} and the proof is complete. ∎

3.5 Change of group functors

In this subsection, we discuss the several change of group functors connecting the KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} categories we defined earlier. The key features of these functors are that they are defined already at the level of algebras, and fit in useful adjunctions upon passing to the KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} categories. Note that it would also have been possible to develop the (dual) Green-Julg adjunctions in this framework, but we omit it since we do not have to put it to use.

We begin by defining the relevant functors at the level of algebras

Definition 3.12.

Let H,GH,G be locally compact, second countable groups.

  1. 1.

    Let φ:H→G\varphi:H\rightarrow G be a continuous homomorphism2121 21 not necessarily inclusion of a subgroup. Then we have the obvious restriction functor

    resHG:𝖦𝖢∗​𝖠𝗅𝗀sep→𝖧𝖢∗​𝖠𝗅𝗀sep.\operatorname{res}^{G}_{H}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.
  2. 2.

    When H⊆GH\subseteq G is closed, we define the induction functor

    indHG:𝖧𝖢∗​𝖠𝗅𝗀sep→𝖦𝖢∗​𝖠𝗅𝗀sep\operatorname{ind}^{G}_{H}:\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}

    as follows:

    • •

      On objects, indHG\operatorname{ind}^{G}_{H} sends B∈𝖧𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to the invariant C∗C^{*}-subalgebra of Cb​(G,B)C_{b}(G,B) (the group GG acts on Cb​(G,B)C_{b}(G,B) by (g,f)⟼(g′↦f⁡(g−1​g′))(g,f)\longmapsto(g^{\prime}\mapsto f(g^{-1}g^{\prime})); note that this action is not neccesarily continuous, but it will be so on indHG⁡(B)\operatorname{ind}^{G}_{H}(B)) generated by the functions f:G→Bf:G\rightarrow B satisfying

      f(gh)=h−1f(g)∀h∈H,∀g∈G&projection ofsupp(f)toG/His compact.f(gh)=h^{-1}f(g)\penalty\ \forall h\in H,\forall g\in G\penalty\ \penalty\ \&\penalty\ \penalty\ \text{projection of}\penalty\ \operatorname{supp}(f)\penalty\ \text{to}\penalty\ G/H\penalty\ \text{is compact}.
    • •

      On morphisms, indHG\operatorname{ind}^{G}_{H} sends a morphism φ:B→B′\varphi:B\rightarrow B^{\prime} in 𝖧𝖢∗​𝖠𝗅𝗀sep\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to

      indHG⁡(φ):indHG⁡(B)→indHG⁡(B′)\operatorname{ind}^{G}_{H}(\varphi):\operatorname{ind}^{G}_{H}(B)\rightarrow\operatorname{ind}^{G}_{H}(B^{\prime})

      given by (indHG⁡(φ)​(f))​(g):=φ⁡(f⁡(g))(\operatorname{ind}^{G}_{H}(\varphi)(f))(g):=\varphi(f(g)).

  3. 3.

    When H⊆GH\subseteq G is closed and G/HG/H is compact, then we also call the associated induction functor as the coinduction functor, and is denoted by 𝖼𝗈𝗂𝗇𝖽HG\mathsf{coind}^{G}_{H}.2222 22 the coinduction functor can be defined under more general conditions, but we do not have any reason to do so.

Remark 3.12.

Note that resG\operatorname{res}^{G} denotes the underlying non-equivariant C∗C^{*}-algebra functor, and resG\operatorname{res}_{G} denotes the functor which equips a (non-equivariant) C∗C^{*}-algebra with the trivial GG-action (we usually omit the trivial group from the notation). Similar comment also applies to the functors resC2G2\operatorname{res}^{G_{2}}_{C_{2}} and resG2C2\operatorname{res}^{C_{2}}_{G_{2}}.

Proposition 3.12.

All the functors defined above descend essentially uniquely to the respective equivariant KK!,∞sepKK_{!,\infty}^{\operatorname{sep}}-categories. Furthermore, the descended functors preserve countable colimits.

Proof.

This can be extracted from [13, Section 4] and [16, Section 2.1]; no comparison with classical bivariant KK-theories is made in loc.​ cit.​ to show that the functors descend, and the proof therein is based on universal properties which we have enforced by construction. Note that the last assertion follows from the universal property of the equivariant KK!,∞sepKK_{!,\infty}^{\operatorname{sep}}-category as described in Section 3.4.5. ∎

Remark 3.12.

Note that the restriction functor has a symmetric monoidal refinement for every choice of (?,!)(?,!) except (?,!)=(min,ex)(?,!)=(\min,\operatorname{ex}), see [13, Corollary 4.8]. The same is not true for the induction or coinduction functors, as can be seen by looking at the unit.

For the next result, we have to provide proofs without banking on classical bivariant KK-theories. Compare [16, Example 2.6]. Note that in all the adjunctions in this article, the left-adjoint is written on the left and the right-adjoint is written on the right.

Proposition 3.12.

If H⊆GH\subseteq G is open2323 23 recall that open subgroups of topological groups are automatically closed, then we have an adjunction

indHG:𝖲𝒦H​𝖧𝖢∗​𝖠𝗅𝗀hsep⇆𝖲𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep:resHG.\operatorname{ind}^{G}_{H}:\mathsf{S}_{\mathcal{K}_{H}}\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\;\leftrightarrows\;\mathsf{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}:\operatorname{res}^{G}_{H}.
Proof.

We begin by the description of the unit and the co-unit.

The unit will be the natural transformation ε:id→𝗋𝖾𝗌HG∘𝗂𝗇𝖽HG\varepsilon:\operatorname{id}\rightarrow\mathsf{res}^{G}_{H}\circ\mathsf{ind}^{G}_{H} with

εA:A\displaystyle\varepsilon_{A}:A →𝗋𝖾𝗌HG​𝗂𝗇𝖽HG​(A)\displaystyle\rightarrow\mathsf{res}^{G}_{H}\mathsf{ind}^{G}_{H}(A)
a\displaystyle a ↦χH​(g)​αg−1​a={αg−1​aif​g∈H0otherwise\displaystyle\mapsto\chi_{H}(g)\alpha_{g^{-1}}a=\begin{cases}\alpha_{g^{-1}}a&\text{if}\penalty\ g\in H\\ 0&\text{otherwise}\end{cases}
2424 24 this is just notation. AA is a HH-C∗C^{*}-algebra, so the action by a general element g−1g^{-1} in GG doesn’t make sense. However, this will only be considered when g−1∈Hg^{-1}\in H.

The description of the co-unit η:𝗂𝗇𝖽HG∘𝗋𝖾𝗌HG→id\eta:\mathsf{ind}^{G}_{H}\circ\mathsf{res}^{G}_{H}\rightarrow\operatorname{id} is more complicated. It is easy to see that

𝗂𝗇𝖽HG​(𝗋𝖾𝗌HG​(B))≅C0​(G/H)⊗B\mathsf{ind}^{G}_{H}(\mathsf{res}^{G}_{H}(B))\cong C_{0}(G/H)\otimes B

Upon representing C0​(G/H)C_{0}(G/H) in ℬ​(L2​(G/H))\mathcal{B}(L^{2}(G/H)) as multiplication operators, C0​(G/H)C_{0}(G/H) factors through 𝒦​(L2​(G/H))\mathcal{K}(L^{2}(G/H)) since G/HG/H is discrete, courtesy HH being open in GG. We can now define the co-unit maps by

ηB:𝗂𝗇𝖽HG​(𝗋𝖾𝗌HG​(B))≅C0​(G/H)⊗B→𝒦⁡(L2​(G/H))⊗B≃B.\eta_{B}:\mathsf{ind}^{G}_{H}(\mathsf{res}^{G}_{H}(B))\cong C_{0}(G/H)\otimes B\rightarrow\mathcal{K}(L^{2}(G/H))\otimes B\simeq B.

It remains to check the triangle identities. We have that the composite

𝗋𝖾𝗌HG\displaystyle\mathsf{res}^{G}_{H} (B)→ε𝗋𝖾𝗌HG​(B)𝗋𝖾𝗌HG​(𝗂𝗇𝖽HG​(𝗋𝖾𝗌HG​(B)))→𝗋𝖾𝗌HG​(ηB)𝗋𝖾𝗌HG​(B)\displaystyle(B)\xrightarrow{\varepsilon_{\mathsf{res}^{G}_{H}(B)}}\mathsf{res}^{G}_{H}(\mathsf{ind}^{G}_{H}(\mathsf{res}^{G}_{H}(B)))\xrightarrow{\mathsf{res}^{G}_{H}(\eta_{B})}\mathsf{res}^{G}_{H}(B)

maps

𝗋𝖾𝗌HG​(B)∋b\displaystyle\mathsf{res}^{G}_{H}(B)\ni b ⟼g↦χH​(g)​βg−1​(b)\displaystyle\longmapsto g\mapsto\chi_{H}(g)\beta_{g^{-1}}(b)
⟼g​H↦χH​(g)​βg​βg−1​(b)\displaystyle\longmapsto gH\mapsto\chi_{H}(g)\beta_{g}\beta_{g^{-1}}(b)
=g​H↦χH​(g)​b\displaystyle=gH\mapsto\chi_{H}(g)b
⟼χH⊗b∈𝗋𝖾𝗌HG​(𝒦⁡(L2​(G/H))⊗B)\displaystyle\longmapsto\chi_{H}\otimes b\in\mathsf{res}^{G}_{H}(\mathcal{K}(L^{2}(G/H))\otimes B)
⟻b,\displaystyle\longmapsfrom b,

where the last map is a left-upper corner inclusion. Note that as a HH-C∗C^{*}-algebra, 𝒦​(L2​(G/H))\mathcal{K}(L^{2}(G/H)) has the trivial action. It follows that

𝗋𝖾𝗌HG​(ηB)∘ε𝗋𝖾𝗌HG​(B)≃id𝗋𝖾𝗌HG​(B).\mathsf{res}^{G}_{H}(\eta_{B})\circ\varepsilon_{\mathsf{res}^{G}_{H}(B)}\simeq\operatorname{id}_{\mathsf{res}^{G}_{H}(B)}.

The analysis of the other composite is more subtle. We have that the composite

𝗂𝗇𝖽HG​(A)→𝗂𝗇𝖽HG​(εA)𝗂𝗇𝖽HG​(𝗋𝖾𝗌HG​(𝗂𝗇𝖽HG​(A)))→η𝗂𝗇𝖽HG​(A)𝗂𝗇𝖽HG​(A)\mathsf{ind}^{G}_{H}(A)\xrightarrow{\mathsf{ind}^{G}_{H}(\varepsilon_{A})}\mathsf{ind}^{G}_{H}(\mathsf{res}^{G}_{H}(\mathsf{ind}^{G}_{H}(A)))\xrightarrow{\eta_{\mathsf{ind}^{G}_{H}(A)}}\mathsf{ind}^{G}_{H}(A)

maps

𝗂𝗇𝖽HG​(A)∋(g↦f⁡(g))\displaystyle\mathsf{ind}^{G}_{H}(A)\ni(g\mapsto f(g)) ⟼(g↦(l↦χH​(l)​αl−1​f​(g)))∈𝗂𝗇𝖽HG​(𝗋𝖾𝗌HG​(𝗂𝗇𝖽HG​(A)))\displaystyle\quad\longmapsto(g\mapsto(l\mapsto\chi_{H}(l)\alpha_{l^{-1}}f(g)))\in\mathsf{ind}^{G}_{H}(\mathsf{res}^{G}_{H}(\mathsf{ind}^{G}_{H}(A)))
⟼(g​H↦(l↦χH​(g−1​l)​α(g−1​l)−1​f​(g)))∈C0​(G/H,indHG⁡(A))\displaystyle\quad\longmapsto(gH\mapsto(l\mapsto\chi_{H}(g^{-1}l)\alpha_{(g^{-1}l)^{-1}}f(g)))\in C_{0}(G/H,\operatorname{ind}^{G}_{H}(A))
=(g​H↦(l↦χH​(g−1​l)​f​(l)))∈C0​(G/H,indHG⁡(A))\displaystyle\quad=(gH\mapsto(l\mapsto\chi_{H}(g^{-1}l)f(l)))\in C_{0}(G/H,\operatorname{ind}^{G}_{H}(A))
↦(†)∑k​H∈G/Hχk​H⊗χk​H​f∈𝒦⁡(L2​(G/H))⊗𝗂𝗇𝖽HG​(A)​(see Section 3.5 below)\displaystyle\quad\xmapsto{(\dagger)}\sum_{kH\in G/H}\chi_{kH}\otimes\chi_{kH}f\in\mathcal{K}(L^{2}(G/H))\otimes\mathsf{ind}^{G}_{H}(A)\penalty\ \text{(see \lx@cref{creftypecap~refnum}{lem: technical manipulation} below)}

It remains to analyse the fate of ∑k​H∈G/Hχk​H⊗χk​H​f\sum_{kH\in G/H}\chi_{kH}\otimes\chi_{kH}f under the equivalences

𝒦⁡(L2​(G/H))⊗𝗂𝗇𝖽HG​(A)→≃𝒦⁡(ℂ⊕L2​(G/H))⊗𝗂𝗇𝖽HG​(A)←≃𝗂𝗇𝖽HG​(A).\mathcal{K}(L^{2}(G/H))\otimes\mathsf{ind}^{G}_{H}(A)\xrightarrow{\simeq}\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H))\otimes\mathsf{ind}^{G}_{H}(A)\xleftarrow{\simeq}\mathsf{ind}^{G}_{H}(A).

We will be done if we can prove the following

Claim.

The two homomorphisms 𝗂𝗇𝖽HG​(A)→𝒦⁡(ℂ⊕L2​(G/H))⊗𝗂𝗇𝖽HG​(A)\mathsf{ind}^{G}_{H}(A)\rightarrow\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H))\otimes\mathsf{ind}^{G}_{H}(A) given by

f↦∑k​H∈G/Hχk​H⊗χk​H​ff\mapsto\sum_{kH\in G/H}\chi_{kH}\otimes\chi_{kH}f

and

f↦p⊗ff\mapsto p\otimes f

are homotopic, where p∈𝒦⁡(ℂ⊕L2​(G/H))p\in\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H)) is the projection onto the summand ℂ\mathbb{C}.

Proof.

Let i:𝒦⁡(L2​(G/H))→𝒦⁡(ℂ⊕L2​(G/H))i:\mathcal{K}(L^{2}(G/H))\xrightarrow{}\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H)) denote the embedding. Then, i⁡(χk​H)∈𝒦⁡(ℂ⊕L2​(G/H))i(\chi_{kH})\in\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H)) is a (not GG-equivariant) one-dimensional projection. It is elementary to see that there is a rank-one partial isometry u∈𝒦⁡(ℂ⊕L2​(G/H))u\in\mathcal{K}(\mathbb{C}\oplus L^{2}(G/H)) such that u​p​u∗=i⁡(χe​H)upu^{*}=i(\chi_{eH}). Defining uk:=k​uu_{k}:=ku, we also have uk​p​uk∗=i⁡(χk​H)u_{k}pu_{k}^{*}=i(\chi_{kH}). Our sought after homotopy is then given by the following one-parameter family of GG-equivariant homomorphisms

φt:𝗂𝗇𝖽HG​(A)\displaystyle\varphi_{t}:\mathsf{ind}^{G}_{H}(A) →𝒦⁡(L2​(G/H))⊗𝗂𝗇𝖽HG​(A)\displaystyle\rightarrow\mathcal{K}(L^{2}(G/H))\otimes\mathsf{ind}^{G}_{H}(A)
f\displaystyle\quad f ↦Σk​H∈G/H(cos(π2t)2i(χk​H)+sin(π2t)2p+cos(π2t)sin(π2t)(uk+uk∗))⊗χk​Hf.\displaystyle\mapsto\underset{kH\in G/H}{\Sigma}(\cos(\frac{\pi}{2}t)^{2}i(\chi_{kH})+\sin(\frac{\pi}{2}t)^{2}p+\cos(\frac{\pi}{2}t)\sin(\frac{\pi}{2}t)(u_{k}+u_{k}^{*}))\otimes\chi_{kH}f.

∎

This finishes the proof of the proposition. ∎

Remark 3.12.

We give here details of the map labelled (†)(\dagger) in the last proof.

On the one hand, we have

g​H⟼\displaystyle gH\longmapsto (l↦χH​(g−1​l)​f​(l))=(l↦χg​H​(l)​f​(l))\displaystyle(l\mapsto\chi_{H}(g^{-1}l)f(l))=(l\mapsto\chi_{gH}(l)f(l))

On the other hand, under the identification C0​(G/H)⊗indHG⁡(A)≅C0​(G/H,indHG⁡(A))C_{0}(G/H)\otimes\operatorname{ind}^{G}_{H}(A)\cong C_{0}(G/H,\operatorname{ind}^{G}_{H}(A)), we have

∑k​H∈G/H​χk​H⊗χk​H​f\underset{{kH\in G/H}}{\sum}\chi_{kH}\otimes\chi_{kH}f

corresponds to the map

gH⟼(l↦∑k​H∈G/Hχk​H(g).χk​H(l)f(l)).\displaystyle gH\longmapsto(l\mapsto\underset{kH\in G/H}{\sum}\chi_{kH}(g).\chi_{kH}(l)f(l)).

On a fixed g​H∈G/HgH\in G/H, both the functions take the value f⁡(l)f(l) if l∈g​Hl\in gH, and 00 otherwise.

Theorem 3.13.

Let H⊆GH\subseteq G be open. Then we have an adjunction

indGH:KKH,sep!,∞⇆KKG,sep!,∞:resGH.\operatorname{ind}^{G}_{H}:\mathrm{KK}^{H,\mathrm{sep}}_{!,\infty}\;\leftrightarrows\;\mathrm{KK}^{G,\mathrm{sep}}_{!,\infty}:\operatorname{res}^{G}_{H}.

Let H⊆GH\subseteq G be closed and G/HG/H be compact. Then we have an adjunction

resGH:KKG,sep!,∞⇆KKH,sep!,∞:𝖼𝗈𝗂𝗇𝖽GH.\operatorname{res}^{G}_{H}:\mathrm{KK}^{G,\mathrm{sep}}_{!,\infty}\;\leftrightarrows\;\mathrm{KK}^{H,\mathrm{sep}}_{!,\infty}:\mathsf{coind}^{G}_{H}.
Proof.

The first statement follows directly from Section 3.5 and Section 3.5, since adjunctions descend to a Dwyer-Kan localization if functors do.

The second statement also follows from Section 3.5 since we have already have an adjunction

resHG:𝖦𝖢∗​𝖠𝗅𝗀sep⇆𝖧𝖢∗​𝖠𝗅𝗀sep:𝖼𝗈𝗂𝗇𝖽HG.\operatorname{res}^{G}_{H}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\;\leftrightarrows\;\mathsf{H}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}:\mathsf{coind}^{G}_{H}.

at the level of algebras (see [6, Lemma 4.2]). For our ease of reference later, we mention the unit and counit of this adjunction here:

ηA:\displaystyle\eta_{A}: A→𝖼𝗈𝗂𝗇𝖽HG​𝗋𝖾𝗌HG​(A),a↦η⁡(a):=(G∋t↦t​a∈A)\displaystyle A\rightarrow\mathsf{coind}^{G}_{H}\mathsf{res}^{G}_{H}(A),\penalty\ \penalty\ a\mapsto\eta(a):=(G\ni t\mapsto ta\in A)
ϵB:\displaystyle\epsilon_{B}: 𝗋𝖾𝗌HG​𝖼𝗈𝗂𝗇𝖽HG​(B)→B,f↦ϵB​(f):=f⁡(1).\displaystyle\mathsf{res}^{G}_{H}\mathsf{coind}^{G}_{H}(B)\rightarrow B,\penalty\ \penalty\ f\mapsto\epsilon_{B}(f):=f(1).

∎

3.6 Connection to KK-theories

In this subsection, we show that the mapping spaces in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} can be understood completely when in the first variable we plug in certain “special” algebras. Consequently, we recover the classical as well as graded, GG-equivariant KK-theory spaces as described in Section 2 as the infinite loop spaces of the mapping spectrum out of ℂ\mathbb{C} and 𝒮\mathcal{S} in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} respectively; see Theorem 3.14.

Since we do not yet know that KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} is an ∞\infty-categorical refinement of the classical bivariant KK-categories, the results of these subsection are crucial for nevertheless being able to make connections to KK-theory, which we use heavily in Section 5.

We now introduce the notion of a !!-special C∗C^{*}-algebra. In what follows, GG is a compact group.

Definition 3.13.

A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is called !!-special if it satisfies the following three conditions2525 25 The H in the enumeration below stands for Hypothesis!.

  1. 1.

    For any !!-exact sequence 0→B→C→D→00\rightarrow B\rightarrow C\rightarrow D\rightarrow 0 in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the induced map

    Map𝖦𝖢∗​𝖠𝗅𝗀hsep⁡(A,B⊗𝒦G)→Map𝖦𝖢∗​𝖠𝗅𝗀hsep⁡(A,C⊗𝒦G)→Map𝖦𝖢∗​𝖠𝗅𝗀hsep⁡(A,D⊗𝒦G)\operatorname{Map}_{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,B\otimes{\mathcal{K}_{G}})\rightarrow\operatorname{Map}_{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,C\otimes{\mathcal{K}_{G}})\rightarrow\operatorname{Map}_{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,D\otimes{\mathcal{K}_{G}})

    is a fiber sequence in Anima.

  2. 2.

    The natural map of abelian monoids

    ⊕n∈ℕ[A,Bn⊗𝒦G]G→[A,⊕n∈ℕ(Bn⊗𝒦G)]G\oplus_{n\in\mathbb{N}}[A,B_{n}\otimes{\mathcal{K}_{G}}]_{G}\rightarrow[A,\oplus_{n\in\mathbb{N}}(B_{n}\otimes{\mathcal{K}_{G}})]_{G}

    is an isomorphism for all countable collection of algebras {Bn}n∈ℕ\{B_{n}\}_{n\in\mathbb{N}} in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

  3. 3.

    The abelian monoid of stable GG-homotopy classes of maps [A,B⊗𝒦G]G[A,B\otimes{\mathcal{K}_{G}}]_{G} is a group for all B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

Remark 3.13.

Clearly, ex−special⟹se−special\operatorname{ex-special}\implies\operatorname{se-special}. In the algebras we consider, we will be showing that they are ex−special\operatorname{ex-special}.

H1 will be satisfied if the induced map of topological spaces

Hom¯G​(A,B)→Hom¯G​(A,C)→Hom¯G​(A,D)\underline{\operatorname{Hom}}_{G}(A,B)\rightarrow\underline{\operatorname{Hom}}_{G}(A,C)\rightarrow\underline{\operatorname{Hom}}_{G}(A,D)

is a Serre fibration of topological spaces for every !!-exact sequence 0→B→C→D→00\rightarrow B\rightarrow C\rightarrow D\rightarrow 0. Indeed, this follows since −⊗𝒦G-\otimes{\mathcal{K}_{G}} is an exact functor on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, and because the ∞\infty-category 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} is presented by the topologically enriched category 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}; see Section 3.1.1.

Similarly, a sufficient criterion to check H2 is that the functor

[A,−]G:𝖦𝖢∗​𝖠𝗅𝗀sep→Set[A,-]_{G}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\operatorname{Set}

preserves countable filtered colimits. This is because countable direct sums can be written as a filtered colimit of finite direct sums, and the functor [A,−]G[A,-]_{G} clearly preserves finite direct sums of algebras in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

The reason we care about !!-special algebras is the following result.

Proposition 3.13.

If A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is !−special\operatorname{!-special}, then

  1. 1.

    The functor

    mapS𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep⁡(A,−):S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep→𝐂𝐌𝐨𝐧⁡(An)\operatorname{map}_{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,-):\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathbf{CMon}(\operatorname{An})

    takes values in 𝐂𝐆𝐫𝐩⁡(An)\mathbf{CGrp}(\operatorname{An}).

  2. 2.

    The functor

    FA:=mapS𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep⁡(A,−):S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep→𝐂𝐆𝐫𝐩⁡(An)F_{A}:=\operatorname{map}_{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,-):\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\rightarrow\mathbf{CGrp}(\operatorname{An})

    factors through KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} (necessarily essentially uniquely) as the functor

    τ≥0mapKK!,∞G,sep(A,−):KK!,∞G,sep→𝐂𝐆𝐫𝐩(An)\tau_{\geq 0}\operatorname{map}_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}(A,-):\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}\rightarrow\mathbf{CGrp}(\operatorname{An})
  3. 3.

    For each B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, there exists a natural equivalence in 𝐂𝐆𝐫𝐩⁡(An)\mathbf{CGrp}(\operatorname{An})

    mapS𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep(A,B)→≃τ≥0mapKK!,∞G,sep(A,B)\operatorname{map}_{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}(A,B)\xrightarrow{\simeq}\tau_{\geq 0}\operatorname{map}_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}(A,B)
Proof.

Assertion 1 is an immediate consequence of H3 and the fact that being a commutative group is a property of a commutative monoid which is furthermore tested on π0\pi_{0}.

To show Assertion 2, we first show that we have a factorization of FAF_{A} as indicated by the dashed arrows below.

S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep{\lx@inpgf@ignorespaces{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}}}𝐂𝐆𝐫𝐩⁡(An){\lx@inpgf@ignorespaces{\mathbf{CGrp}(\operatorname{An})}}S𝒦G𝖦𝖢∗𝖠𝗅𝗀h,!,⊕sep{\lx@inpgf@ignorespaces{\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus}^{\mathrm{sep}}}}KK!,∞G,sep{\lx@inpgf@ignorespaces{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}}FA\scriptstyle{\lx@inpgf@ignorespaces F_{A}}L!,⊕ω\scriptstyle{\lx@inpgf@ignorespaces L_{!,\oplus_{\omega}}}FA′\scriptstyle{\lx@inpgf@ignorespaces F_{A}^{\prime}}LBott\scriptstyle{\lx@inpgf@ignorespaces L_{\mathrm{Bott}}}FA′′\scriptstyle{\lx@inpgf@ignorespaces F_{A}^{\prime\prime}}

To see that FA′F_{A}^{\prime} exists, we bring Section 3.3.3 into play. We need to check that FAF_{A} is left-exact, inverts W^!\hat{W}_{!} and preserves countable coproducts. Being a corepresentable functor, FAF_{A} is clearly left-exact. That it inverts W^!\hat{W}_{!} follows directly from H1 in presence of Equation 3.6. That FAF_{A} also preserves countable coproducts is a consequence of H2, as can be seen from the Whitehead’s theorem for spectra together with the fact that filtered colimits of spectra commute with finite limits. To now see that FA′′F_{A}^{\prime\prime} exists, we simply use Section 3.4.4.

That the factorizations FA′F_{A}^{\prime} and FA′′F_{A}^{\prime\prime} are essentially unique follows from the fact that L!,⊕ωL_{!,\oplus_{\omega}} and LBottL_{\operatorname{Bott}} are Dwyer-Kan localizations. That FA′F_{A}^{\prime} and FA′′F_{A}^{\prime\prime} are also corepresentable by AA follows since the left-Kan extension of a corepresentable functor is corepresentable ([45, Corollary 8.3.1.9]), and in our case, FA′F_{A}^{\prime} and FA′′F_{A}^{\prime\prime} are also left-Kan extensions of FAF_{A} along the localization maps.

Assertion 3 also follows from the previous paragraph. ∎

As an immediate consequence of Assertion 3 of Section 3.6 and the Eckmann-Hilton argument we have the following corollary (cf. [25, Remark 3.24]).

Corollary 3.13.

For any !!-special algebra AA and any B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we have an weak homotopy equivalence of spaces

Hom¯G(A,B⊗𝒦G)≃Ω∞mapKK!,∞G,sep(A,B).\underline{\operatorname{Hom}}_{G}(A,B\otimes\mathcal{K}_{G})\simeq\Omega^{\infty}\operatorname{map}_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}(A,B).

Moreover, under the above equivalence, the block-sum addition on [A,B⊗𝒦G]G[A,B\otimes\mathcal{K}_{G}]_{G} coincides with the additive structure on π0(mapKK!,∞G,sep(A,B))\pi_{0}(\operatorname{map}_{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}(A,B)).

The next two lemmas show that 𝒮\mathcal{S} and q​ℂq\mathbb{C} are ex-special.

Lemma 3.13.

𝒮∈𝖦2​𝖢∗​𝖠𝗅𝗀sep\mathcal{S}\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is ex−special\operatorname{ex-special}.

Proof.

The necessary verifications are the content of the first three assertions of Theorem 2.3. Note that we are implicitly using that the C∗C^{*}-algebra of compact operators on a Hilbert space is inner graded. ∎

Lemma 3.13.

q​ℂ∈𝖦𝖢∗​𝖠𝗅𝗀sepq\mathbb{C}\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} is ex−special\operatorname{ex-special}.

Proof.

That q​ℂq\mathbb{C} satisfies H3 follows from the fact that [q​ℂ,B⊗𝒦G]G[q\mathbb{C},B\otimes{\mathcal{K}_{G}}]_{G} is naturally isomorphic to the abelian group K0G​(B)K^{G}_{0}(B). Since K0G​(−)K^{G}_{0}(-) is known to preserve filtered colimits (for example, by combining Assertion 3 and Assertion 6 of Theorem 2.3), q​ℂq\mathbb{C} also satisfies H2.

That q​ℂq\mathbb{C} satisfies H1 can be shown directly, but we instead deduce it from Section 3.6. To that end, we leverage the isomorphism of C∗C^{*}-algebras q​ℂ≅(𝒮​⊗^​C​l0,1)uq\mathbb{C}\cong(\mathcal{S}\hat{\otimes}Cl^{0,1})_{u} as mentioned in Section 2.1.5. The rest follows from the fact that 𝒮\mathcal{S} satisfies H1 for the group G2G_{2} and the restriction-coinduction adjunction. In more detail, for any B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we have natural equivalences

S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep​(q​ℂ,B)\displaystyle\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}(q\mathbb{C},B) ≃S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep​(𝗋𝖾𝗌GG2​(𝒮​⊗^​C​l0,1),B)\displaystyle\simeq\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\!\left(\mathsf{res}^{G_{2}}_{G}(\mathcal{S}\hat{\otimes}Cl^{0,1}),B\right)
≃𝖲𝒦G2​𝖦2​𝖢∗​𝖠𝗅𝗀hsep​(𝒮​⊗^​C​l0,1,B​⊗^​C​l0,1)\displaystyle\simeq\mathsf{S}_{\mathcal{K}_{G_{2}}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\!\left(\mathcal{S}\hat{\otimes}Cl^{0,1},B\hat{\otimes}Cl^{0,1}\right)
→≃⊗^​C​l1,0𝖲𝒦G2​𝖦2​𝖢∗​𝖠𝗅𝗀hsep​(𝒮,B).\displaystyle\xrightarrow[\simeq]{\hat{\otimes}Cl^{1,0}}\mathsf{S}_{\mathcal{K}_{G_{2}}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}(\mathcal{S},B).

Note that for the second equivalence, we are using the identification2626 26 the more well known isomorphism is with the ungraded tensor product, but since BB has the trivial C2C_{2}-action, we can also use the graded tensor product. 𝖼𝗈𝗂𝗇𝖽GG2​B≅B​⊗^​C​l0,1\mathsf{coind}^{G_{2}}_{G}B\cong B\hat{\otimes}Cl^{0,1}. For the final equivalence, we are also using that the graded tensor products ⊗^!\hat{\otimes}_{!} on 𝖦2​𝖢∗​𝖠𝗅𝗀sep\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} also descend to a symmetric monoidal structure on 𝖲𝒦G2​𝖦2​𝖢∗​𝖠𝗅𝗀hsep\mathsf{S}_{\mathcal{K}_{G_{2}}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}, which is easy to see since the algebras of continuous functions on the unit interval and compact operators on a Hilbert space are inner graded. ∎

Remark 3.13.

We note that ℂ\mathbb{C} is not !!-special, as H3 fails for it. We mention without proof that C0​(ℝ0,1)C_{0}(\mathbb{R}^{0,1}) is !!-special.

Finally, we obtain the following important connection between classical models of equivariant and graded KK-theories and the infinite loop spaces of the mapping spectrum in the stable ∞\infty-categories we constructed, as mentioned at the beginning of this subsection.

Theorem 3.14.

We have natural equivalences of spaces for any B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and B^∈𝖦2​𝖢∗​𝖠𝗅𝗀sep\hat{B}\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}:

𝕂G(B)≃Ω∞KK!,∞G,sep(ℂ,B),𝕂^G(B^)≃Ω∞KK!,∞G2,sep(𝒮,B^).\mathbb{K}^{G}(B)\simeq\Omega^{\infty}\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}(\mathbb{C},B),\qquad\mathbb{\hat{K}}^{G}(\hat{B})\simeq\Omega^{\infty}\mathrm{KK}_{!,\infty}^{G_{2},\mathrm{sep}}(\mathcal{S},\hat{B}).

Moreover, K0G(−),KK!,0G,sep(ℂ,−):𝖦𝖢∗𝖠𝗅𝗀sep→AbK_{0}^{G}(-),\mathrm{KK}_{!,0}^{G,\mathrm{sep}}(\mathbb{C},-):\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\operatorname{Ab} are equivalent as lax monoidal functors, where KK!,0G,sep(ℂ,−)\mathrm{KK}_{!,0}^{G,\mathrm{sep}}(\mathbb{C},-) denotes the homotopy category of KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}.

Proof.

The first two assertions follow from Section 3.6 and the last two lemmas. For the first assertion we are also using that q​ℂq\mathbb{C} and ℂ\mathbb{C} are equivalent in KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}, as follows from Section 3.4.1. The last assertion follows from the lax case of Section 3.4.9. ∎

3.7 Extension to all C∗C^{*}-algebras

In this subsection, we construct presentable stable ∞\infty-categories KKG!,∞\mathrm{KK}^{G}_{!,\infty} which contain KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} as its full subcategory of ℵ1\aleph_{1}-compact objects.

Definition 3.14.

Denote by

KK!,∞G:=Indℵ1(KK!,∞G,sep),\mathrm{KK}^{G}_{!,\infty}:=\operatorname{Ind}_{\aleph_{1}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}),

where Indℵ1⁡(𝒞)\operatorname{Ind}_{\aleph_{1}}(\mathcal{C}) denotes the ℵ1\aleph_{1}-ind completion of 𝒞\mathcal{C}, i.e. the category obtained by freely adding2727 27 see [43, Proposition 5.3.5.10] for the precise universal property ℵ1\aleph_{1}-filtered colimits to 𝒞\mathcal{C}. We define functors

kkG!,∞:𝖦𝖢∗𝖠𝗅𝗀→KKG!,∞\mathrm{kk}^{G}_{!,\infty}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\mathrm{KK}^{G}_{!,\infty}

as left Kan-extensions

𝖦𝖢∗​𝖠𝗅𝗀sep{\lx@inpgf@ignorespaces{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}}}KK!,∞G,sep{\lx@inpgf@ignorespaces{\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}}}}KKG!,∞{\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{!,\infty}}}𝖦𝖢∗​𝖠𝗅𝗀{\lx@inpgf@ignorespaces{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}}}kk!,∞G,sep\scriptstyle{\lx@inpgf@ignorespaces\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}}incl.\scriptstyle{\lx@inpgf@ignorespaces\operatorname{incl.}}y\scriptstyle{\lx@inpgf@ignorespaces y}kkG!,∞\scriptstyle{\lx@inpgf@ignorespaces\mathrm{kk}^{G}_{!,\infty}}

where y:𝒞→Indℵ1⁡(𝒞)y:\mathcal{C}\rightarrow\operatorname{Ind}_{\aleph_{1}}(\mathcal{C}) denotes the canonical embedding (which preserves countable filtered colimits by [43, Proposition 5.3.5.14]).

Before studying the general properties of the above construction, we need the following definition and an accompanying lemma.

Definition 3.14.

A functor FF defined on 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg} is called s-finitary if for every A∈𝖦𝖢∗​𝖠𝗅𝗀A\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}, the canonical map

colimA′⊆sepAF(A′)→F(A)\operatorname{colim}_{A^{\prime}\subseteq_{\operatorname{sep}}A}F(A^{\prime})\rightarrow F(A)

is an equivalence, where A′A^{\prime} runs through the separable GG-invariant C∗C^{*}-subalgebras of AA.

Lemma 3.14.

Let F:𝖦𝖢∗​𝖠𝗅𝗀→𝒟F:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\mathcal{D} be a functor to an ∞\infty-category 𝒟\mathcal{D} having all small filtered colimits. We have a canonical natural transformation c:F^⟹Fc:\hat{F}\implies F, where F^\hat{F} is the left Kan extension of F∣𝖦𝖢∗​𝖠𝗅𝗀sepF\mid_{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}}. Then the functor FF is s-finitary if and only if cc is an equivalence.

Proof.

This follows immediately from the pointwise formula for left Kan extension, and the fact that every morphism A→BA\rightarrow B in 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg} with AA separable factors through a GG-invariant separable C∗C^{*}-subalgebra of BB. See [13, Lemma 3.1] for more details. ∎

Proposition 3.14.
  1. 1.

    The category KKG!,∞\mathrm{KK}^{G}_{!,\infty} is a presentably symmetric monoidal (for every choice of (?,!)(?,!) except (min,ex)(\min,\operatorname{ex})), stable ∞\infty-category, and KK!,∞G,sep\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}} can be identified with the full subcategory of KKG!,∞\mathrm{KK}^{G}_{!,\infty} comprising of ℵ1\aleph_{1}-compact objects.

  2. 2.

    The functor kkG!,∞:𝖦𝖢∗𝖠𝗅𝗀→KKG!,∞\mathrm{kk}^{G}_{!,\infty}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\mathrm{KK}^{G}_{!,\infty} is symmetric monoidal (for every choice of (?,!)(?,!) except (min,ex)(\min,\operatorname{ex})), homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, !!-exact, preserves countable direct sums and is s-finitary2828 28 note that any functor on 𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg} which preserves countable direct sums and is s-finitary automatically preserves all direct sums..

  3. 3.

    Pullback along kkG!,∞\mathrm{kk}^{G}_{!,\infty} induces for every cocomplete symmetric monoidal stable ∞\infty-category 𝒟\mathcal{D} with bi-cocontinous tensor product an equivalence

    (kk!,∞G)∗:𝐅𝐮𝐧⊗?/laxcolim(KK!,∞G,𝒟)→≃𝐅𝐮𝐧⊗?/laxh,𝒦G,!,⊕ω,sfin(𝖦𝖢∗𝖠𝗅𝗀,𝒟),(\mathrm{kk}^{G}_{!,\infty})^{*}:\mathbf{Fun}^{\operatorname{colim}}_{\otimes_{?}\operatorname{/lax}}(\mathrm{KK}^{G}_{!,\infty},\mathcal{D})\xrightarrow{\simeq}\mathbf{Fun}^{h,{\mathcal{K}_{G}},\operatorname{!},\oplus_{\omega},\operatorname{sfin}}_{\otimes_{?}\operatorname{/lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg},\mathcal{D}),

    where the superscript sfin\operatorname{sfin} denotes s-finitary functors.

Proof.

Assertion 1 follows from the general fact that if 𝒞\mathcal{C} is a small, symmetric monoidal, κ\kappa-cocomplete (for some regular cardinal κ\kappa), stable ∞\infty-category such that the tensor product preserves κ\kappa-small colimits in each variable, then Indκ⁡(𝒞)\operatorname{Ind}_{\kappa}(\mathcal{C}) is a presentably symmetric monoidal stable ∞\infty-category and 𝒞\mathcal{C} can be identified with the full subcategory of Indκ⁡(𝒞)\operatorname{Ind}_{\kappa}(\mathcal{C}) comprising of ℵ1\aleph_{1}-compact objects. See [43, Theorem 5.5.1.1], [44, Proposition 1.1.3.6] and [44, Corollary 4.8.1.14].

The proof of Assertion 2 can be taken from [13, Theorem 1.18] and [13, Proposition 3.8]2929 29 the proof of lax monoidality of kkG!,∞\mathrm{kk}^{G}_{!,\infty} is formal, but to show its (strong) monoidality, one has to look into the structure of the minimal and maximal tensor products; see loc.​ cit.​ for details. Note that although [13] is written with Indℵ0\operatorname{Ind}_{\aleph_{0}}-completion, all the filtered diagrams considered in Section 3 of loc.​ cit.​ are indeed ℵ1\aleph_{1}-filtered, and so the proofs go through in our context too. The Real and the (potentially) non-discrete group case do not pose any difficulties.

Assertion 3 follows from the series of equivalences

𝐅𝐮𝐧colim⊗?/lax(KKG!,∞,𝒟)\displaystyle\mathbf{Fun}^{\operatorname{colim}}_{\otimes_{?}\operatorname{/lax}}(\mathrm{KK}^{G}_{!,\infty},\mathcal{D}) →≃y∗𝐅𝐮𝐧colimω⊗?/lax(KK!,∞G,sep,𝒟)\displaystyle\xrightarrow[\simeq]{y^{*}}\mathbf{Fun}^{\operatorname{colim}_{\omega}}_{\otimes_{?}\operatorname{/lax}}(\mathrm{KK}_{!,\infty}^{G,\mathrm{sep}},\mathcal{D})
→≃kk!,∞G,sep∗𝐅𝐮𝐧h,𝒦G,!,⊕ω⊗?/lax(𝖦𝖢∗𝖠𝗅𝗀sep,𝒟)\displaystyle\xrightarrow[\simeq]{{\mathrm{kk}_{!,\infty}^{G,\mathrm{sep}}}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},!,\oplus_{\omega}}_{\otimes_{?}\operatorname{/lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},\mathcal{D})
←≃incl∗𝐅𝐮𝐧h,𝒦G,!,⊕ω,sfin⊗?/lax(𝖦𝖢∗𝖠𝗅𝗀,𝒟).\displaystyle\xleftarrow[\simeq]{\operatorname{incl}^{*}}\mathbf{Fun}^{h,{\mathcal{K}_{G}},!,\oplus_{\omega},\operatorname{sfin}}_{\otimes_{?}\operatorname{/lax}}(\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg},\mathcal{D}).

where the first equivalence follows from [43, Proposition 5.3.5.10] and [44, Corollary 4.8.1.14], the second equivalence is the content of Section 3.4.9, and the last equivalence follows from Section 3.7 and Assertion 2. Note that the inverse to the last equivalence is precisely the left Kan-extension along the inclusion 𝖦𝖢∗​𝖠𝗅𝗀sep→incl.𝖦𝖢∗​𝖠𝗅𝗀\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\xrightarrow{\operatorname{incl.}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}. ∎

The next result is a generalization of Theorem 3.14 to the non-separable case.

Theorem 3.15.

We have natural equivalences of spaces for any B∈𝖦𝖢∗​𝖠𝗅𝗀B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg} and B^∈𝖦2​𝖢∗​𝖠𝗅𝗀\hat{B}\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}:

𝕂G(B)≃Ω∞KK!,∞G(ℂ,B),𝕂^G(B^)≃Ω∞KK!,∞G2(𝒮,B^).\mathbb{K}^{G}(B)\simeq\Omega^{\infty}\mathrm{KK}^{G}_{!,\infty}(\mathbb{C},B),\qquad\mathbb{\hat{K}}^{G}(\hat{B})\simeq\Omega^{\infty}\mathrm{KK}^{G_{2}}_{!,\infty}(\mathcal{S},\hat{B}).

Moreover, K0G(−),KK!,0G(ℂ,−):𝖦𝖢∗𝖠𝗅𝗀→AbK_{0}^{G}(-),\mathrm{KK}^{G}_{!,0}(\mathbb{C},-):\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\operatorname{Ab} are equivalent as lax monoidal functors, where KKG!,0\mathrm{KK}^{G}_{!,0} denotes the homotopy category of KKG!,∞\mathrm{KK}^{G}_{!,\infty}.

Proof.

This follows immediately from Theorem 3.14 upon noting that all the relevant functors preserve ℵ1\aleph_{1}-filtered colimits. ∎

Corollary 3.15.

KK!,0C2(𝒮,𝒮)≅ℤ⁡[x]x2=1\mathrm{KK}^{C_{2}}_{!,0}(\mathcal{S},\mathcal{S})\cong\frac{\mathbb{Z}[x]}{x^{2}=1} as rings, with the preferred isomorphism mapping [1𝒮][\operatorname{1}_{\mathcal{S}}] to 11, and [α𝒮][\alpha_{\mathcal{S}}] to xx. For any graded C∗C^{*}-algebra AA, the action of αA\alpha_{A} on K^0​(A)\hat{K}_{0}(A) coincides with the action of α𝒮∈KK!,0C2(𝒮,𝒮)\alpha_{\mathcal{S}}\in\mathrm{KK}^{C_{2}}_{!,0}(\mathcal{S},\mathcal{S}) on K^0​(A)\hat{K}_{0}(A) stemming from the product in the KKC2!,0\mathrm{KK}^{C_{2}}_{!,0} category.

Proof.

This is immediate from Assertion 8 of Section 2.2 and Theorem 3.15. ∎

Remark 3.15.

The second perspective in Section 3.7 directly shows why even the boundary maps in the long exact sequences of graded KK-theory groups preserve the action of the grading (and this is because of the associativity of composition in the KKC2!,0\mathrm{KK}^{C_{2}}_{!,0} category), and hence the associated long exact sequence can be viewed as a long exact sequence of C2C_{2}-abelian groups.

The final result of this section discusses the change of group functors on the categories of all C∗C^{*}-algebras.

Theorem 3.16.

There are obvious analogues of the change of group functors of Section 3.5 to the categories of all C∗C^{*}-algebras. These functors then descend to cocontinuous functors between the respective equivariant KK!,∞KK_{!,\infty}-categories. The restriction functors have symmetric monoidal refinement for every choice of (?,!)(?,!) except for (min,ex)(\min,\operatorname{ex}). If H⊆GH\subseteq G is open, then we have an adjunction

indGH:KKH!,∞⇆KKG!,∞:resGH.\operatorname{ind}^{G}_{H}:\mathrm{KK}^{H}_{!,\infty}\leftrightarrows\mathrm{KK}^{G}_{!,\infty}:\operatorname{res}^{G}_{H}.

If H⊆GH\subseteq G is closed and G/HG/H is compact, then we have an adjunction

resGH:KKG!,∞⇆KKH!,∞:𝖼𝗈𝗂𝗇𝖽GH.\operatorname{res}^{G}_{H}:\mathrm{KK}^{G}_{!,\infty}\leftrightarrows\mathrm{KK}^{H}_{!,\infty}:\mathsf{coind}^{G}_{H}.
Proof.

In light of the results of Section 3.5 and Section 3.7.3, we have to show that the functors 𝗂𝗇𝖽HG​(−),𝗋𝖾𝗌HG​(−),𝖼𝗈𝗂𝗇𝖽HG​(−)\mathsf{ind}^{G}_{H}(-),\mathsf{res}^{G}_{H}(-),\mathsf{coind}^{G}_{H}(-) between the relevant categories of all C∗C^{*}-algebras are s-finitary. But this is contained in [13, Section 4], see also [16, Section 2.1]. ∎

4 Graded, Real KKG!,∞KK^{G}_{!,\infty}-theory

In this section, we define the graded KKG!,∞KK^{G}_{!,\infty}-categories. We follow some ideas from [15] and an unpublished note of Bunke-Duenzinger ([12]). Note that we make our definitions on the large category 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg} from the get go.

It will be ubiquitous for our approach to graded bivariant KK-theories that 𝒮\mathcal{S} is a cocommutative coalgebra (also called comonoid) in (𝖦​𝖢^∗​𝖠𝗅𝗀,⊗^?)(\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg},\widehat{\otimes}_{?}). In what follows, we stop decorating the tensor product because 𝒮\mathcal{S} is nuclear, see [63, Corollary E.2.19]. We first come with a diagonal map 𝒮→𝒮​⊗^​𝒮\mathcal{S}\rightarrow\mathcal{S}\hat{\otimes}\mathcal{S}. The following result is proven in detail in [26, Proposition 4.3].

Proposition 4.0.

There is a unique graded ∗*-homomorphism 𝒮→𝒮​⊗^​𝒮\mathcal{S}\rightarrow\mathcal{S}\hat{\otimes}\mathcal{S} such that

u↦u​⊗^​u,v↦u​⊗^​v+v​⊗^​u,u\mapsto u\hat{\otimes}u,\penalty\ \penalty\ \penalty\ \penalty\ v\mapsto u\hat{\otimes}v+v\hat{\otimes}u,

where u:=e−x2u:=e^{-x^{2}}, v=x​e−x2v=xe^{-x^{2}}.

We also have a graded ∗*-homomorphism η:𝒮→ℂ\eta:\mathcal{S}\rightarrow\mathbb{C}, given by η⁡(f)=f⁡(0)\eta(f)=f(0).

Corollary 4.0.

The ∗*-homomorphisms η\eta and △\triangle equip 𝒮\mathcal{S} with a cocommutative coalgebra structure; in the sense that the following diagrams commute

𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}}}𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}}}𝒮​⊗^​𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}\hat{\otimes}\mathcal{S}}}𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}}}𝒮​⊗^​𝒮{\lx@inpgf@ignorespaces{\mathcal{S}\hat{\otimes}\mathcal{S}}}Δ\scriptstyle{\lx@inpgf@ignorespaces\Delta}Δ\scriptstyle{\lx@inpgf@ignorespaces\Delta}1​⊗^​Δ\scriptstyle{\lx@inpgf@ignorespaces 1\hat{\otimes}\Delta}flip\scriptstyle{\lx@inpgf@ignorespaces\operatorname{flip}}=\scriptstyle{\lx@inpgf@ignorespaces=}=\scriptstyle{\lx@inpgf@ignorespaces=}Δ\scriptstyle{\lx@inpgf@ignorespaces\Delta}Δ\scriptstyle{\lx@inpgf@ignorespaces\Delta}Δ\scriptstyle{\lx@inpgf@ignorespaces\Delta}Δ​⊗^​1\scriptstyle{\lx@inpgf@ignorespaces\Delta\hat{\otimes}1}η​⊗^​1\scriptstyle{\lx@inpgf@ignorespaces\eta\hat{\otimes}1}1​⊗^​η\scriptstyle{\lx@inpgf@ignorespaces 1\hat{\otimes}\eta}
Proof.

This is immediate by considering the elements uu and vv in 𝒮\mathcal{S}. ∎

Lemma 4.0.

KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty} has a presentably symmetric monoidal structure for the graded tensor products ⊗^?\hat{\otimes}_{?} for every choice of (?,!)(?,!) except (?,!)=(min,ex)(?,!)=(\min,\operatorname{ex}), and the canonical functor 𝖦2𝖢∗𝖠𝗅𝗀→KKG2!,∞\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}\rightarrow\mathrm{KK}^{G_{2}}_{!,\infty} has a symmetric monoidal refinement too.

Proof.

We just discuss the separable analogue of the statement; the generalization to the large categories is a routine argument in light of the results of Section 3.7.

One checks directly that each of the steps in the localizations

𝖦2𝖢∗𝖠𝗅𝗀sep→Lh𝖦2𝖢∗𝖠𝗅𝗀hsep→L𝒦G2S𝒦G2𝖦2𝖢∗𝖠𝗅𝗀hsep→L!,⊕S𝒦G2𝖦2𝖢∗𝖠𝗅𝗀h,!,⊕ωsep→LBottKK!,∞G2,sep.\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\xrightarrow{L_{h}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{\mathcal{K}_{G_{2}}}}\mathrm{S}_{\mathcal{K}_{G_{2}}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}}\xrightarrow{L_{!,\oplus}}\mathrm{S}_{\mathcal{K}_{G_{2}}}\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}_{h,!,\oplus_{\omega}}^{\mathrm{sep}}\xrightarrow{L_{\operatorname{Bott}}}\mathrm{KK}_{!,\infty}^{G_{2},\mathrm{sep}}.

has a symmetric monoidal refinement for the graded tensor products, since under the restrictions imposed on (?,!)(?,!), it is clear that at each step A⊗^!−A\hat{\otimes}_{!}- preserves the class of morphisms that are inverted at that step (to see this for the excision step, we use that the underlying Banach spaces of the graded and ungraded tensor products coincide, see [63, Lemma E.2.18]). The rest of the details are exactly as in the ungraded case. ∎

Notation 4.0.

Henceforth whenever we mention symmetric monoidal structures on equivariant KK!,∞KK_{!,\infty} categories, we consider all choices of (?,!)(?,!) except (?,!)=(min,ex)(?,!)=(\min,\operatorname{ex}). We also stop decorating the tensor product every time; the decoration is implicitly assumed to be there abiding by the exception mentioned in the previous sentence.

We now proceed with the task of defining symmetric monoidal bivariant KK-categories for 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}. We achieve this by defining KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} as a full subcategory of the category of comodules over 𝒮\mathcal{S} in KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty}. In general, if (𝒞,⊗)(\cal{C},\otimes) is any presentably symmetric monoidal category with a cocommutative coalgebra object 𝒮\mathcal{S}, then we have an adjunction

forget:𝐂𝐨𝐦𝐨𝐝𝒞(𝒮)⇆𝒞:𝒮⊗−\operatorname{forget}:\mathbf{Comod}_{\mathcal{C}}(\mathcal{S})\leftrightarrows\mathcal{C}:\mathcal{S}\otimes-

where 𝐂𝐨𝐦𝐨𝐝𝒞​(𝒮)\mathbf{Comod}_{\mathcal{C}}(\mathcal{S}) denotes the presentable ∞\infty-category of comodules over 𝒮\mathcal{S}, and 𝒮⊗−\mathcal{S}\otimes- denotes the cofree comodule functor. The details of this can be found in [44, Section 4.2.4]. 3030 30 Note that use of the word (co)free is not analogous to the use of the word free as in “free abelian group on a set”, and should not create any confusion! We mention that the proof of presentability of the category of comodules is subtle (see [50, Proposition 3.8]), and was explained to the author by Maxime Ramzi.

The next definition should be read together with the remarks following it.

Definition 4.0.

The graded bivariant KKG!KK^{G}_{!}-category, denoted KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}, is the full subcategory spanned by cofree comodules in 𝐂𝐨𝐦𝐨𝐝KKG2!,∞(𝒮)\mathbf{Comod}_{\mathrm{KK}^{G_{2}}_{!,\infty}}(\mathcal{S}). Note that KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} becomes a symmetric monoidal category with respect to the balanced tensor product of comodules ([44, Section 4.4]).

Denote by kk^G!,∞\widehat{\mathrm{kk}}^{G}_{!,\infty} the composition of the symmetric monoidal functors

kk^G!,∞:𝖦𝖢^∗𝖠𝗅𝗀→kkG2!,∞KKG2!,∞→𝒮​⊗^−KK^G!,∞\widehat{\mathrm{kk}}^{G}_{!,\infty}:\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}\xrightarrow{\mathrm{kk}^{G_{2}}_{!,\infty}}\mathrm{KK}^{G_{2}}_{!,\infty}\xrightarrow{\mathcal{S}\hat{\otimes}-}\widehat{\mathrm{KK}}^{G}_{!,\infty}\
Remark 4.0.

The following remarks about Section 4 are in order.

  1. 1.

    Explicitly written out, the relative tensor product of 𝒮​⊗^​A\mathcal{S}\hat{\otimes}A and 𝒮​⊗^​B\mathcal{S}\hat{\otimes}B is 𝒮​⊗^​A​⊗^​B\mathcal{S}\hat{\otimes}A\hat{\otimes}B, with the codiagonal map 𝒮→Δ𝒮​⊗^​𝒮\mathcal{S}\xrightarrow{\Delta}\mathcal{S}\hat{\otimes}\mathcal{S} being used to cancel out one action of 𝒮\mathcal{S}. This also roughly shows why KKG2!,∞→𝒮​⊗^−KK^G!,∞\mathrm{KK}^{G_{2}}_{!,\infty}\xrightarrow{\mathcal{S}\hat{\otimes}-}\widehat{\mathrm{KK}}^{G}_{!,\infty} is symmetric monoidal.

  2. 2.

    It is not clear if the category KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} is stable, since cofree comodules need not be closed under the formation of finite limits or colimits. Nevertheless, it is enriched over Spectra being the full subcategory of a stable ∞\infty-category, as follows from the next point.

  3. 3.

    At first glance, a natural solution to the above problem could seem to simply work with the category of all 𝒮\mathcal{S}-comodules. But then, there is no reason for this category to be symmetric monoidal, since one does not have appropriate commutation of the tensor product with cosimplicial limits in general (necessary for the dual of [44, Theorem 4.5.2.1] to be applicable). Note that the monoidality assertions in [15, Definition 2.45] are incorrect.

  4. 4.

    In applications, it is more important to have symmetric monoidality of the graded bivariant KK-categories than having presentability. Therefore we choose the definition above.

  5. 5.

    Denote by KK^G!,0\widehat{\mathrm{KK}}^{G}_{!,0} the homotopy category of KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}. From the forgetful-cofree adjunction, we immediately get the hom groups in KK^G!,0\widehat{\mathrm{KK}}^{G}_{!,0} are given by

    KK^!,0G(A,B)≅KK!,0G2(𝒮⊗^A,B).{\widehat{\mathrm{KK}}^{G}_{!,0}}(A,B)\cong{\mathrm{KK}^{G_{2}}_{!,0}}(\mathcal{S}\hat{\otimes}A,B).

    The composite of φ∈KK^!,0G(A,B)≅KK!,0G2(𝒮⊗^A,B)\varphi\in\widehat{\mathrm{KK}}^{G}_{!,0}(A,B)\cong\mathrm{KK}^{G_{2}}_{!,0}(\mathcal{S}\hat{\otimes}A,B) and ψ∈KK^!,0G(B,C)≅KK!,0G2(𝒮⊗^B,C)\psi\in\widehat{\mathrm{KK}}^{G}_{!,0}(B,C)\cong\mathrm{KK}^{G_{2}}_{!,0}(\mathcal{S}\hat{\otimes}B,C) is given by the composite in KKG2!,0\mathrm{KK}^{G_{2}}_{!,0}

    𝒮​⊗^​A→Δ​⊗^​1A𝒮​⊗^​𝒮​⊗^​A→1𝒮​⊗^​φ𝒮​⊗^​B→𝜓C.\mathcal{S}\hat{\otimes}A\xrightarrow{\Delta\hat{\otimes}1_{A}}\mathcal{S}\hat{\otimes}\mathcal{S}\hat{\otimes}A\xrightarrow{1_{\mathcal{S}}\hat{\otimes}\varphi}\mathcal{S}\hat{\otimes}B\xrightarrow{\psi}C.

    The functor

    kk^G!,0:𝖦𝖢^∗𝖠𝗅𝗀→KK^G!,0\widehat{\mathrm{kk}}^{G}_{!,0}:\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}\rightarrow\widehat{\mathrm{KK}}^{G}_{!,0}

    is identity on objects and precomposes with 𝒮​⊗^​A→ev0∗A\mathcal{S}\hat{\otimes}A\xrightarrow{{\operatorname{ev}_{0}}_{*}}A on morphisms emanating out of AA.

We now mention important by-products of our definitions. These will be crucially used in the next section.

Proposition 4.0.

If A,B∈𝖦​𝖢^∗​𝖠𝗅𝗀A,B\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg} are equivalent in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}, then 𝒮​⊗^​A\mathcal{S}\hat{\otimes}A and 𝒮​⊗^​B\mathcal{S}\hat{\otimes}B are equivalent in KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty}.

Proof.

By Section 4, AA and BB are equivalent in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} means that we have an equivalence

kk!,∞G2(𝒮)⊗^kk!,∞G2(A)≃kk!,∞G2(𝒮)⊗^kk!,∞G2(B)\mathrm{kk}^{G_{2}}_{!,\infty}(\mathcal{S})\hat{\otimes}\mathrm{kk}^{G_{2}}_{!,\infty}(A)\simeq\mathrm{kk}^{G_{2}}_{!,\infty}(\mathcal{S})\hat{\otimes}\mathrm{kk}^{G_{2}}_{!,\infty}(B)

of cofree comodules. Invoking the functoriality of the forgetful functor 𝐂𝐨𝐦𝐨𝐝KKG2!,∞(𝒮)→KK!,∞G2\mathbf{Comod}_{\mathrm{KK}^{G_{2}}_{!,\infty}}(\mathcal{S})\rightarrow\mathrm{KK}^{G_{2}}_{!,\infty} now finishes the argument. ∎

Theorem 4.1.

For any B^∈𝖦​𝖢^∗​𝖠𝗅𝗀\hat{B}\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}, we have a natural equivalence of spaces

𝕂^G(B^)≃Ω∞KK^!,∞G(ℂ,B^).\mathbb{\hat{K}}^{G}(\hat{B})\simeq\Omega^{\infty}\widehat{\mathrm{KK}}^{G}_{!,\infty}(\mathbb{C},\hat{B}).

Moreover, K^0G(−),KK^!,0G(ℂ,−):𝖦𝖢^∗𝖠𝗅𝗀⟶Ab\hat{K}_{0}^{G}(-),\;\widehat{\mathrm{KK}}^{G}_{!,0}(\mathbb{C},-):\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}\longrightarrow\operatorname{Ab} are equivalent as lax monoidal functors.

Proof.

This is an immediate consequence of Section 4, Theorem 3.15, and Theorem 2.3.4. The lax monoidality assertion follows upon observing that the lax monoidality of KK!,∞G2(𝒮,−)\mathrm{KK}^{G_{2}}_{!,\infty}(\mathcal{S},-) stems from the codiagonal map 𝒮→Δ𝒮​⊗^​𝒮\mathcal{S}\xrightarrow{\Delta}\mathcal{S}\hat{\otimes}\mathcal{S} too, as mentioned in Section 4.1. ∎

We now show that graded KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}-theories recover ungraded KKG!,∞\mathrm{KK}^{G}_{!,\infty}-theories when the algebras are trivially graded. More precisely,

Theorem 4.2.

In the commutative square

𝖦𝖢∗​𝖠𝗅𝗀{\lx@inpgf@ignorespaces{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}}}KKG!,∞{\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{!,\infty}}}𝖦​𝖢^∗​𝖠𝗅𝗀{\lx@inpgf@ignorespaces{\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}}}KKG2!,∞{\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{!,\infty}}}KK^G!,∞{\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}^{G}_{!,\infty}}}kkG!,∞\scriptstyle{\lx@inpgf@ignorespaces\mathrm{kk}^{G}_{!,\infty}}𝗋𝖾𝗌G2G​(−)\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G}_{G_{2}}(-)}𝗋𝖾𝗌G2G​(−)\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G}_{G_{2}}(-)}𝒮​⊗^​𝗋𝖾𝗌G2G​(−)\scriptstyle{\lx@inpgf@ignorespaces\mathcal{S}\hat{\otimes}\mathsf{res}^{G}_{G_{2}}(-)}kkG2!,∞\scriptstyle{\lx@inpgf@ignorespaces\mathrm{kk}^{G_{2}}_{!,\infty}}𝒮​⊗^−\scriptstyle{\lx@inpgf@ignorespaces\mathcal{S}\hat{\otimes}-}

the right functor is fully faithful.

Proof.

We have to show that the composite

KK!,∞G(A,B)→𝗋𝖾𝗌G2G​(−)KK!,∞G2(𝗋𝖾𝗌G2G(A),𝗋𝖾𝗌G2G(B))→ev0∗KK!,∞G2(𝒮⊗^𝗋𝖾𝗌G2G(A),𝗋𝖾𝗌G2G(B))\mathrm{KK}^{G}_{!,\infty}(A,B)\xrightarrow{\mathsf{res}^{G}_{G_{2}}(-)}\mathrm{KK}^{G_{2}}_{!,\infty}(\mathsf{res}^{G}_{G_{2}}(A),\mathsf{res}^{G}_{G_{2}}(B))\xrightarrow{\operatorname{ev}_{0}^{*}}\mathrm{KK}^{G_{2}}_{!,\infty}(\mathcal{S}\hat{\otimes}\mathsf{res}^{G}_{G_{2}}(A),\mathsf{res}^{G}_{G_{2}}(B)) (4.3)

is an equivalence. To that end, we accommodate Equation 4.3 into the commutative diagram (note that the left part of the diagram commutes can be seen by explicitly calculating the fate of a GG-equivariant homomorphism from AA to BB using the definition of the unit of the restriction-coinduction adjunction as described in Section 3.5. The formulae of loc.​ cit.​ also work in the non-separable case)

KK!,∞G(A,B){\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{!,\infty}(A,B)}}KK!,∞G2(𝗋𝖾𝗌G2G(A),𝗋𝖾𝗌G2G(B)){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{!,\infty}\!\left(\mathsf{res}^{G}_{G_{2}}(A),\mathsf{res}^{G}_{G_{2}}(B)\right)}}KK!,∞G2(𝒮⊗^𝗋𝖾𝗌G2G(A),𝗋𝖾𝗌G2G(B)){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{!,\infty}\!\left(\mathcal{S}\hat{\otimes}\mathsf{res}^{G}_{G_{2}}(A),\mathsf{res}^{G}_{G_{2}}(B)\right)}}KK!,∞G2(𝗋𝖾𝗌G2G(A)⊗^Cl0,1,𝗋𝖾𝗌G2G(B)⊗^Cl0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{!,\infty}\!\left(\mathsf{res}^{G}_{G_{2}}(A)\hat{\otimes}Cl^{0,1},\mathsf{res}^{G}_{G_{2}}(B)\hat{\otimes}Cl^{0,1}\right)}}KK!,∞G2(𝒮⊗^𝗋𝖾𝗌G2G(A)⊗^Cl0,1,𝗋𝖾𝗌G2G(B)⊗^Cl0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{!,\infty}\!\left(\mathcal{S}\hat{\otimes}\mathsf{res}^{G}_{G_{2}}(A)\hat{\otimes}Cl^{0,1},\mathsf{res}^{G}_{G_{2}}(B)\hat{\otimes}Cl^{0,1}\right)}}KK!,∞G(𝗋𝖾𝗌GG2(A⊗Cl0,1),B){\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{!,\infty}\!\left(\mathsf{res}^{G_{2}}_{G}(A\otimes Cl^{0,1}),B\right)}}KK!,∞G(𝗋𝖾𝗌GG2(𝒮⊗^Cl0,1)⊗A,B){\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{!,\infty}\!\left(\mathsf{res}^{G_{2}}_{G}(\mathcal{S}\hat{\otimes}Cl^{0,1})\otimes A,B\right)}}𝗋𝖾𝗌G2G​(−)\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G}_{G_{2}}(-)}(C​lu0,1→π1ℂ)∗\scriptstyle{\lx@inpgf@ignorespaces(Cl^{0,1}_{u}\xrightarrow{\pi_{1}}\mathbb{C})^{*}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}^{*}}−⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}Cl^{0,1}}−⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}Cl^{0,1}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}^{*}}𝗋𝖾𝗌GG2⊣𝖼𝗈𝗂𝗇𝖽GG2\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G_{2}}_{G}\dashv\mathsf{coind}^{G_{2}}_{G}}𝗋𝖾𝗌GG2⊣𝖼𝗈𝗂𝗇𝖽GG2\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G_{2}}_{G}\dashv\mathsf{coind}^{G_{2}}_{G}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}^{*}}

Note that we implicitly have used that AA and BB have the trivial grading so as to replace some graded tensor products with the ungraded ones. In light of the above diagram, our thesis would follow once we have shown that the composite

(𝒮​⊗^​C​l0,1)u→ev0∗C​lu0,1→π1ℂ(\mathcal{S}\hat{\otimes}Cl^{0,1})_{u}\xrightarrow{{\operatorname{ev}_{0}}_{*}}Cl^{0,1}_{u}\xrightarrow{\pi_{1}}\mathbb{C}

is an equivalence in KKG!,∞\mathrm{KK}^{G}_{!,\infty}. But this readily follows from Section 3.4.3.

∎

4.1 The Bott map in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} and consequences

We can now export results from [26, Section 9] in our setup. We begin with the definition of the Bott class. For VV any Euclidean vector space equipped with a self-adjoint involution (VV was called a pseudo Euclidean vector space in [26, Section 9.1]), we denote by 𝒞⁡(V)\mathcal{C}(V) the graded C∗C^{*}-algebra C0​(V,C​l​(V))C_{0}(V,Cl(V)). For the next few results, we do not consider the external group GG.

Definition 4.3.

Let VV be a pseudo Euclidean vector space. Let ι:V→C​l​(V)\iota:V\rightarrow Cl(V) denote the canonical inclusion of VV into C​l​(V)Cl(V). Then the functional calculus of ι\iota yields a graded homomorphism

bV:𝒮→𝒞⁡(V),b_{V}:\mathcal{S}\rightarrow\mathcal{C}(V),

which we call the Bott map. It naturally determines a point in the spectral KK-theory space 𝕂^​(𝒞​(V)),\mathbb{\hat{K}}\bigl(\mathcal{C}(V)\bigr), and hence also a point in Ω∞KK^!,∞(ℂ,𝒞(V)).\Omega^{\infty}\widehat{\mathrm{KK}}_{!,\infty}\bigl(\mathbb{C},\mathcal{C}(V)\bigr). In light of Theorem 4.1, we denote either of them by bVb_{V}.

Remark 4.3.

[26, Section 9] contains a detailed proof that π0​𝕂^​(𝒞⁡(V))≅ℤ\pi_{0}\hat{\mathbb{K}}\bigl(\mathcal{C}(V)\bigr)\cong\mathbb{Z}, and that bVb_{V} is a generator of this group. Consequently, bVb_{V} is also a generator of π0mapKK^!,∞(ℂ,𝒞(V))≅ℤ\pi_{0}\operatorname{map}_{\widehat{\mathrm{KK}}_{!,\infty}}\bigl(\mathbb{C},\mathcal{C}(V)\bigr)\cong\mathbb{Z}. Furthermore, the proof of Section 2.2.4 shows that

bV×bV¯∈π0​𝕂^​(𝒞⁡(V)​⊗^​𝒞​(V¯))≅π0​𝕂^​(𝒞⁡(V⊕V¯))≅ℤb_{V}\times b_{\overline{V}}\in\pi_{0}\hat{\mathbb{K}}\bigl(\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V})\bigr)\cong\pi_{0}\hat{\mathbb{K}}(\mathcal{C}(V\oplus\overline{V}))\cong\mathbb{Z}

is a generator of the group.

We end this subsection with a technical lemma. Although the result is an immediate corollary of Theorem 4.4, we need the lemma in the proof of it, and so must have it a priori.

Lemma 4.3.

For any pseudo-Euclidean vector space VV, the morphism

bV×bV¯∈KK^!,0(ℂ,𝒞(V)⊗^𝒞(V¯))b_{V}\times b_{\overline{V}}\in\widehat{\mathrm{KK}}_{!,0}\bigl(\mathbb{C},\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V})\bigr)

is an isomorphism in KK^!,0\widehat{\mathrm{KK}}_{!,0}.

Proof.

Section 4.1 shows that bV×bV¯b_{V}\times b_{\overline{V}} is a unit in KK^!,0(ℂ,𝒞(V)⊗^𝒞(V¯))\widehat{\mathrm{KK}}_{!,0}(\mathbb{C},\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V})). On the other hand, the Toeplitz extension theory shows that there is a KK^!,0\widehat{\mathrm{KK}}_{!,0}-equivalence between ℂ\mathbb{C} and 𝒞⁡(V)​⊗^​𝒞​(V¯)\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V}), given by the image of the boundary map of the Toeplitz extension under the canonical functor KKC2!,0→KK^!,0\mathrm{KK}^{C_{2}}_{!,0}\rightarrow\widehat{\mathrm{KK}}_{!,0}. This also has to be a unit in ℤ\mathbb{Z} because of the following general fact: in any additive 11-category 𝒟\mathcal{D}, if there are isomorphic objects xx and yy such that hom𝒟⁡(x,y)≅ℤ\operatorname{hom}_{\mathcal{D}}(x,y)\cong\mathbb{Z} as abelian groups, then the isomorphism necessarily corresponds to ±1\pm 1.3131 31 a proof of this fact can be deduced from the elementary algebra fact that any commutative unital ring structure on the abelian group ℤ\mathbb{Z} must be isomorphic to the standard ring structure on ℤ\mathbb{Z} ([1, Exercise 2.16]). To prove our thesis, we simply use that if ff is an isomorphism in an additive category, then so is −f-f. ∎

We next prove the following result, which is well known in the classical frameworks of K​KKK- and EE-theory; see [39], [40], [32]. We remind the reader that we do not yet know that our KK^!,0\widehat{\mathrm{KK}}_{!,0} categories are equivalent to classical graded K​KKK- or EE-categories, and hence need to give an independent proof.

Theorem 4.4.

For any pseudo Euclidean vector space VV, the Bott element bVb_{V} is an equivalence in KK^!,0\widehat{\mathrm{KK}}_{!,0}.

We now build up to the proof of Theorem 4.4. We start off by spelling out the interchange law in a monoidal (∞\infty)-categories.

Lemma 4.4.

Let 𝒞\mathcal{C} be a monoidal (∞)(\infty)-category, and let A,B,C,A′,B′,C′A,B,C,A^{\prime},B^{\prime},C^{\prime} be objects of 𝒞\mathcal{C}. For composable morphisms

A→𝑓B→𝑔C,A′→ℎB′→𝑘C′,A\xrightarrow{f}B\xrightarrow{g}C,\qquad A^{\prime}\xrightarrow{h}B^{\prime}\xrightarrow{k}C^{\prime},

the functoriality of the tensor product ⊗:𝒞×𝒞⟶𝒞\otimes:\mathcal{C}\times\mathcal{C}\longrightarrow\mathcal{C} gives a canonical homotopy

(g∘f)⊗(k∘h)≃(g⊗k)∘(f⊗h)(g\circ f)\otimes(k\circ h)\simeq(g\otimes k)\circ(f\otimes h)

in the mapping space Map𝒞⁡(A⊗A′,C⊗C′).\operatorname{Map}_{\mathcal{C}}(A\otimes A^{\prime},\,C\otimes C^{\prime}).

Lemma 4.4.

For any X∈𝖢^∗​𝖠𝗅𝗀X\in\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}, the following diagram of abelian groups commutes

KK^!,0(𝒞(V),X){\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}_{!,0}(\mathcal{C}(V),X)}}KK^!,0(ℂ,X){\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}_{!,0}(\mathbb{C},X)}}KK^!,0(𝒞(V)⊗^𝒞(V¯),X⊗^𝒞(V¯)){\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}_{!,0}\bigl(\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V}),X\hat{\otimes}\mathcal{C}(\overline{V})\bigr)}}KK^!,0(ℂ,X⊗^𝒞(V¯)){\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}_{!,0}\bigl(\mathbb{C},X\hat{\otimes}\mathcal{C}(\overline{V})\bigr)}}KK^!,0(ℂ,X){\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}_{!,0}(\mathbb{C},X)}}bV∗\scriptstyle{\lx@inpgf@ignorespaces b_{V}^{*}}−⊗^​𝒞​(V¯)\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}\mathcal{C}(\overline{V})}=\scriptstyle{\lx@inpgf@ignorespaces=}(bV×bV¯)∗\scriptstyle{\lx@inpgf@ignorespaces(b_{V}\times b_{\overline{V}})^{*}}−×bV¯\scriptstyle{\lx@inpgf@ignorespaces-\times b_{\overline{V}}} (4.5)

Furthermore, all the arrows in the above diagram are isomorphisms.

Proof.

That all the morphisms in the diagram are additive is clear. That it also commutes is an application of Section 4.1. In the notation of loc.​ cit.​ we take

𝒞:=KK^!,0,A=A′=ℂ,B=𝒞(V),B′=C′=𝒞(V¯),C=X.\mathcal{C}:=\widehat{\mathrm{KK}}_{!,0},A=A^{\prime}=\mathbb{C},B=\mathcal{C}(V),B^{\prime}=C^{\prime}=\mathcal{C}(\overline{V}),C=X.

As for the morphisms, we can take any g∈KK^!,0(𝒞(V),X)g\in\widehat{\mathrm{KK}}_{!,0}(\mathcal{C}(V),X), and

f=bV,h=bV¯,k=id𝒞⁡(V¯).f=b_{V},h=b_{\overline{V}},k=\operatorname{id}_{\mathcal{C}(\overline{V})}.

Since Equation 4.5 commutes, it suffices to show that the two left vertical arrows and the bottom horizontal arrows are isomorphisms. That

−⊗^𝒞(V¯):KK^!,0(𝒞(V),X)→KK^!,0(𝒞(V)⊗^𝒞(V¯),X⊗^𝒞(V¯))-\hat{\otimes}\mathcal{C}(\overline{V}):\widehat{\mathrm{KK}}_{!,0}(\mathcal{C}(V),X)\rightarrow\widehat{\mathrm{KK}}_{!,0}(\mathcal{C}(V)\hat{\otimes}\mathcal{C}(\overline{V}),X\hat{\otimes}\mathcal{C}(\overline{V}))

is an isomorphism follows because tensoring with 𝒞⁡(V¯)\mathcal{C}(\overline{V}) yields an isomorphism in KKC2!,0\mathrm{KK}^{C_{2}}_{!,0} (with the inverse being tensoring with 𝒞⁡(V)\mathcal{C}(V)), and because the cofree comodule functor KKC2!,∞→𝒮​⊗^−KK^!,∞\mathrm{KK}^{C_{2}}_{!,\infty}\xrightarrow{\mathcal{S}\hat{\otimes}-}\widehat{\mathrm{KK}}_{!,\infty} is symmetric monoidal. That bV×bV¯b_{V}\times b_{\overline{V}} is an isomorphism follows from Section 4.1, and the bottom horizontal arrow being an isomorphism is the content of [26, Theorem 9.13]. ∎

Remark 4.5.

We mention that the proof of [26, Theorem 9.13] uses non-trivial functional analysis and features of classical graded KK-theory (such as graded asymptotic morphisms between graded C∗C^{*}-algebras induce morphisms between the graded KK-groups). However, the “KK-theoretic” result is enough for the proof of Section 4.1, and we do not need to know that there is any relation between the KK^!,0\widehat{\mathrm{KK}}_{!,0} categories and asymptotic morphisms. And indeed, when !=se!=\operatorname{se}, a general asymptotic morphism would not induce a morphism in KK^se,0\widehat{\mathrm{KK}}_{\mathrm{se},0}.

Proof of Theorem 4.4.

This readily follows from the Yoneda lemma and Section 4.1. ∎

We next deduce an important corollary of Theorem 4.4. We can now bring back our external compact group GG.

Corollary 4.5.

In KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}, we have an equivalence C0​(V)≃C​l​(V¯)C_{0}(V)\simeq Cl(\overline{V}). In particular, the functor

−⊗^Cl1,0:KK^G!,∞→KK^G!,∞-\hat{\otimes}Cl^{1,0}:\widehat{\mathrm{KK}}^{G}_{!,\infty}\rightarrow\widehat{\mathrm{KK}}^{G}_{!,\infty}

is equivalent to the loops functor on KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}.

Proof.

We begin by first observing that Theorem 4.4 also shows that the Bott element is an equivalence in KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty}. This is because ℂ\mathbb{C} and 𝒞⁡(V)\mathcal{C}(V) have the trivial GG-action, and we have an obvious “equipping with the trivial GG-action” functor KK^!,∞→KK^G!,∞\widehat{\mathrm{KK}}_{!,\infty}\rightarrow\widehat{\mathrm{KK}}^{G}_{!,\infty}.3232 32 More formally, we could have developed a graded variant of the change of group functors, and deduced this from the functoriality of the restriction functor. But because we would not have the occassion to use it anywhere else, we omit the details.

It suffices to show that C0​(V)C_{0}(V) and C​l​(V¯){Cl}(\overline{V}) are isomorphic in KK^G!,0\widehat{\mathrm{KK}}^{G}_{!,0}. But this follows from the implications

ℂ≅𝒞⁡(V)⟹C​l​(V¯)≅C0​(V)​⊗^​C​l​(V)​⊗^​C​l​(V¯)⟹C​l​(V¯)≅C0​(V),\mathbb{C}\cong\mathcal{C}(V)\implies Cl(\overline{V})\cong C_{0}(V)\hat{\otimes}Cl(V)\hat{\otimes}Cl(\overline{V})\implies Cl(\overline{V})\cong C_{0}(V),

where we used that tensoring with C​l​(V¯)Cl(\overline{V}) is already an isomorphism in KKG2!,0\mathrm{KK}^{G_{2}}_{!,0}, and because ℂ→C​l​(V⊕V¯)\mathbb{C}\rightarrow Cl(V\oplus\overline{V}) is a KKG2!,0\mathrm{KK}^{G_{2}}_{!,0}-equivalence.

The last assertion follows from the observation that the canonical functor KKG2!,∞→KK^G!,∞\mathrm{KK}^{G_{2}}_{!,\infty}\rightarrow\widehat{\mathrm{KK}}^{G}_{!,\infty} is left-exact, and loops in KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty} is modeled by C0​(ℝ0,1)C_{0}(\mathbb{R}^{0,1}). ∎

We end this section by showing a fundamental feature (or defect!) of graded KK^!,∞\widehat{\mathrm{KK}}_{!,\infty}-categories. Recall that (equivariant) KK!,∞KK_{!,\infty}-categories for ungraded, separable C∗C^{*} algebras enjoy the universal property of being a Dwyer-Kan localization at certain class of morphisms. We show that the analogous statement for KK^!,∞\widehat{\mathrm{KK}}_{!,\infty} categories is false. This issue seems to not have been discussed anywhere in the literature, and Bunke-Duenzinger left it as an open question (in the complex case) in [12]. The author learnt the crux of the proof from Johannes Ebert. The proof in its present form was suggested by Maxime Ramzi.

Proposition 4.5.

The full subcategory of KK^!,∞\widehat{\mathrm{KK}}_{!,\infty} spanned by separable, graded C∗C^{*}-algebras (denoted KK^!,∞sep\widehat{\mathrm{KK}}_{!,\infty}^{\operatorname{sep}}) is not the Dwyer-Kan localization of the category of separable, graded C∗C^{*}-algebras at any class of morphisms.

Proof.

Since the grading on a graded C∗C^{*}-algebra induces a C2C_{2}-action on the graded KK-groups, we have a commutative diagram of functors

C2​−Ab{\lx@inpgf@ignorespaces{C_{2}\!\operatorname{-Ab}}}𝖢^∗​𝖠𝗅𝗀sep{\lx@inpgf@ignorespaces{\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}}}Ab{\lx@inpgf@ignorespaces{\operatorname{Ab}}}KK^sep!,∞{\lx@inpgf@ignorespaces{\widehat{\mathrm{KK}}^{\mathrm{sep}}_{!,\infty}}}forget\scriptstyle{\lx@inpgf@ignorespaces\operatorname{forget}}K^0​(−)\scriptstyle{\lx@inpgf@ignorespaces\hat{K}_{0}(-)}K^0​(−)\scriptstyle{\lx@inpgf@ignorespaces\hat{K}_{0}(-)}kk^sep!,∞\scriptstyle{\lx@inpgf@ignorespaces\widehat{\mathrm{kk}}^{\mathrm{sep}}_{!,\infty}}π0KK^!,∞sep(ℂ,−)\scriptstyle{\lx@inpgf@ignorespaces\pi_{0}\widehat{\mathrm{KK}}^{\mathrm{sep}}_{!,\infty}(\mathbb{C},-)}

Note that the bottom triangle commutes from Theorem 4.1. But since the forgetful functor C2​−Ab→AbC_{2}\!\operatorname{-Ab}\rightarrow\operatorname{Ab} reflects isomorphisms, had K​K^!,∞sep\widehat{KK}_{!,\infty}^{\operatorname{sep}} been a Dwyer-Kan localization, we would obtain a lift in the above diagram KK^!,∞sep→C2−Ab\widehat{\mathrm{KK}}_{!,\infty}^{\operatorname{sep}}\rightarrow C_{2}\!\operatorname{-Ab}, and thereby conclude that the K^0\hat{K}_{0}-groups of two KK^!,∞sep\widehat{\mathrm{KK}}_{!,\infty}^{\operatorname{sep}}-equivalent C∗C^{*}-algebras are in fact isomorphic as C2C_{2}-abelian groups. In light of Theorem 4.4, this a contradiction, since K^0​(ℂ)≅ℤ\hat{K}_{0}(\mathbb{C})\cong\mathbb{Z} with the trivial C2C_{2}-action, whereas K^0​(C0​(ℝ,C​l0,1))≅ℤ\hat{K}_{0}(C_{0}(\mathbb{R},Cl^{0,1}))\cong\mathbb{Z} with the action n↦−nn\mapsto-n, as shown in Section 2.2.4. ∎

Remark 4.5.

Note that there is an obvious equivariant version of Section 4.1 too.

5 Applications: certain fiber sequences connecting different K-theories

We now use the technology developed in the previous section in order to study the relationships between graded KK-theory, C2C_{2}-equivariant KK-theory and ungraded (classical) KK-theory. All the results can be deduced in the presence of an external compact group GG, as we will be doing. The following remarks are in order.

Remark 5.0.

We will be using the following elementary observations in this section even without mentioning.

  1. 1.

    The datum of a G×HG\times H-action on a C∗C^{*}-algebra AA is same as the datum of a GG-action and a HH-action on AA which commute. Under this identification, it makes sense to talk about the GG- and HH-actions on a (G×H)(G\times H)-C∗C^{*}-algebra. Similar comment also applies to equivariant projective modules. For G2G_{2}-equivariant projective modules, we will be omitting the GG-action from the notation, and just keep track of the C2C_{2}-action. For example, when we write (A,α)∈𝖦2​𝖢∗​𝖠𝗅𝗀(A,\alpha)\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}, we mean the C2C_{2}-action is given by α\alpha.

  2. 2.

    Suppose A,B,C∈𝖦2​𝖢∗​𝖠𝗅𝗀A,B,C\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg} have trivial GG-action, and fit in a fiber sequence in KKC2!,∞\mathrm{KK}^{C_{2}}_{!,\infty}. Then, since resG2C2\operatorname{res}^{C_{2}}_{G_{2}} is left-exact, they also fit in a fiber sequence in KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty}.

  3. 3.

    With Theorem 3.15 and Theorem 4.1 at our disposal, we will henceforth be (abusing notation and) denoting by 𝕂G\mathbb{K}^{G} (resp. 𝕂^G\hat{\mathbb{K}}^{G}) the GG-equivariant (resp. graded GG-equivariant) KK-theory spectra, given by KK!,∞G(ℂ,−)KK_{!,\infty}^{G}(\mathbb{C},-) (resp. KK^!,∞G(ℂ,−)≃KK!,∞G2(𝒮,−)\widehat{\mathrm{KK}}^{G}_{!,\infty}(\mathbb{C},-)\simeq KK_{!,\infty}^{G_{2}}(\mathcal{S},-)). As before, we will be denoting their homotopy groups by K∗G​(−)K_{*}^{G}(-) (resp. K^∗G​(−)\hat{K}_{*}^{G}(-)).

  4. 4.

    In the remainder of this section, we fix a compact group GG. For concreteness, we work with KKex,∞G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty} in this section. The same calculations can also be done with K​Kse,∞G2KK_{\operatorname{se},\infty}^{G_{2}}.

5.1 A fiber sequence connecting the different KK-theory spectra

The low hanging fruit that we can now pluck off is the following. We will be using the shorthand (−)u(-)_{u} to denote the functor resGG2⁡(−)\operatorname{res}^{G_{2}}_{G}(-) (uu stands for the “underlying ungraded C∗C^{*}-algebra”).

Proposition 5.0.

We have a natural fiber sequence of spectra

𝕂G​(Au)→𝕂G2​(A)→𝕂^G​(A)\mathbb{K}^{G}(A_{u})\rightarrow\mathbb{K}^{G_{2}}(A)\rightarrow\hat{\mathbb{K}}^{G}(A) (5.1)

for every A∈𝖦2​𝖢∗​𝖠𝗅𝗀A\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}.

Proof.

Upon applying the exact functor

KKex,∞G2​(−,A):𝖦2​𝖢∗​𝖠𝗅𝗀⟶Sp\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(-,A):\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}\longrightarrow\operatorname{Sp}

to the fiber sequence of Section 3.4.2, we are done once we justify the maps (1)(1), (2)(2), and (3)(3) in the following diagram:

KKex,∞G2​(C​l0,1,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A)}}KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(𝒮,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathcal{S},A)}}𝕂G​(Au){\lx@inpgf@ignorespaces{\mathbb{K}^{G}(A_{u})}}𝕂G2​(A){\lx@inpgf@ignorespaces{\mathbb{K}^{G_{2}}(A)}}𝕂^G​(A){\lx@inpgf@ignorespaces{\hat{\mathbb{K}}^{G}(A)}}ι∗\scriptstyle{\lx@inpgf@ignorespaces\iota^{*}}≃(1)\scriptstyle{\lx@inpgf@ignorespaces\simeq\,(1)}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}^{*}}≃(2)\scriptstyle{\lx@inpgf@ignorespaces\simeq\,(2)}≃(3)\scriptstyle{\lx@inpgf@ignorespaces\simeq\,(3)}

The map labeled (1)(1) arises from the induction-restriction adjunction (Theorem 3.16), since we can identify 𝗂𝗇𝖽GG2​ℂ\mathsf{ind}^{G_{2}}_{G}\mathbb{C} with C​l0,1Cl^{0,1}. The second and third equivalence follow from Theorem 3.15. ∎

In the next two remarks, we explain a couple of different formulations of the fiber sequence in Equation 5.1. Though the above sequence will be our main workhorse, these other formulations come handy in certain cases.

Remark 5.1.

We claim that there is a fiber sequence

𝕂G​(Au)→(A→A​⊗^​C​l0,1)∗𝕂G​((A​⊗^​C​l0,1)u)→𝕂^G​(A)\mathbb{K}^{G}(A_{u})\xrightarrow{(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}}\mathbb{K}^{G}((A\hat{\otimes}Cl^{0,1})_{u})\rightarrow\hat{\mathbb{K}}^{G}(A) (5.2)

which is equivalent to the fiber sequence in Equation 5.1. Indeed, this will follow from the following commutative diagram

KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(C​l0,1,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A)}}KKex,∞G2​(C​l0,1,A​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A\hat{\otimes}Cl^{0,1})}}KKex,∞G​(ℂ,Au){\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u})}}KKex,∞G​(ℂ,(A​⊗^​C​l0,1)u){\lx@inpgf@ignorespaces{\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},(A\hat{\otimes}Cl^{0,1})_{u})}}−⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}Cl^{0,1}}ι∗\scriptstyle{\lx@inpgf@ignorespaces\iota^{*}}(A→A​⊗^​C​l0,1)∗\scriptstyle{\lx@inpgf@ignorespaces(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}}𝗂𝗇𝖽GG2⊣𝗋𝖾𝗌GG2\scriptstyle{\lx@inpgf@ignorespaces\mathsf{ind}^{G_{2}}_{G}\dashv\mathsf{res}^{G_{2}}_{G}}𝗂𝗇𝖽GG2⊣𝗋𝖾𝗌GG2\scriptstyle{\lx@inpgf@ignorespaces\mathsf{ind}^{G_{2}}_{G}\dashv\mathsf{res}^{G_{2}}_{G}}(A→A​⊗^​C​l0,1)∗\scriptstyle{\lx@inpgf@ignorespaces(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}} (5.3)

Note that the top triangle commutes because the diagram below commutes in KKex,∞G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}, where f:C​l0,1→Af:Cl^{0,1}\rightarrow A is any morphism in KKex,∞G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}. The left triangle below does not commute at the level of algebras, but only up to homotopy.

C​l0,1{\lx@inpgf@ignorespaces{Cl^{0,1}}}A{\lx@inpgf@ignorespaces A}C​l0,1{\lx@inpgf@ignorespaces{Cl^{0,1}}}C​l0,2{\lx@inpgf@ignorespaces{Cl^{0,2}}}A​⊗^​C​l0,1{\lx@inpgf@ignorespaces{A\hat{\otimes}Cl^{0,1}}}f\scriptstyle{\lx@inpgf@ignorespaces f}=\scriptstyle{\lx@inpgf@ignorespaces=}1C​l0,1​⊗^​ι\scriptstyle{\lx@inpgf@ignorespaces 1_{Cl^{0,1}}\hat{\otimes}\iota}1A​⊗^​ι\scriptstyle{\lx@inpgf@ignorespaces 1_{A}\hat{\otimes}\iota}ι​⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces\iota\hat{\otimes}Cl^{0,1}}f​⊗^​1C​l0,1\scriptstyle{\lx@inpgf@ignorespaces f\hat{\otimes}1_{Cl^{0,1}}} (5.4)
Remark 5.4.

We claim there is a fiber sequence

𝕂G2​(A​⊗^​C​l1,0)→(A→A​⊗^​C​l1,0)∗𝕂G2​(A)→𝕂^G​(A)\mathbb{K}^{G_{2}}(A\hat{\otimes}Cl^{1,0})\xrightarrow{(A\rightarrow A\hat{\otimes}Cl^{1,0})^{*}}\mathbb{K}^{G_{2}}(A)\rightarrow\hat{\mathbb{K}}^{G}(A) (5.5)

which is equivalent to the fiber sequence in Equation 5.1. The map labeled A→(A​⊗^​C​l1,0)∗A\rightarrow(A\hat{\otimes}Cl^{1,0})^{*} should be taken with a pinch of salt as 𝕂G2​(−)\mathbb{K}^{G_{2}}(-) is naturally covariantly functorial; what we mean is the map obtained from the zig-zag

A​⊗^​C​l1,0→A​⊗^​C​l1,1←≃A.A\hat{\otimes}Cl^{1,0}\rightarrow A\hat{\otimes}Cl^{1,1}\xleftarrow{\simeq}A.

When AA is unital, it can be shown ([3, Section 4.5.2]) that on π0\pi_{0}, this has the same effect as precomposing the structure map of a G2G_{2}-equivariant A​⊗^​C​l1,0A\hat{\otimes}Cl^{1,0} projective module with the homomorphism A→A​⊗^​C​l1,0A\rightarrow A\hat{\otimes}Cl^{1,0}. The equivalence of the fiber sequences in Equation 5.1 and Equation 5.5 can be shown by a similar treatment as in the last remark.

This formulation of the fiber sequence is directly related to the classical Atiyah-Bott-Shapiro description of KK-groups of a point, see Section 5.1 for more details.

Proposition 5.5.

When AA is inner graded, the fiber sequence in Equation 5.1 (and hence also the ones in Equation 5.2 and Equation 5.5) splits.

Proof.

In light of Equation 5.2, we have to show that the map of spectra

KKex,∞G​(ℂ,Au)→(A→A​⊗^​C​l0,1)∗KKex,∞G​(ℂ,(A​⊗^​C​l0,1)u).\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u})\xrightarrow{(A\to A\hat{\otimes}Cl^{0,1})_{*}}\mathrm{KK}^{G}_{\mathrm{ex},\infty}\bigl(\mathbb{C},(A\hat{\otimes}Cl^{0,1})_{u}\bigr).

has a retraction when AA is inner graded. In this case, since A​⊗^​C​l0,1≅A⊗C​l0,1A\hat{\otimes}Cl^{0,1}\cong A\otimes Cl^{0,1} in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}, we can extend the aforementioned map to

KKex,∞G​(ℂ,Au)\displaystyle\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u}) →(A→A​⊗^​C​l0,1)∗KKex,∞G​(ℂ,(A​⊗^​C​l0,1)u)\displaystyle\xrightarrow{(A\to A\hat{\otimes}Cl^{0,1})_{*}}\mathrm{KK}^{G}_{\mathrm{ex},\infty}\bigl(\mathbb{C},(A\hat{\otimes}Cl^{0,1})_{u}\bigr)
→≃KKex,∞G​(ℂ,(A⊗C​l0,1)u)→≃KKex,∞G​(ℂ,Au⊕Au)\displaystyle\xrightarrow{\simeq}\mathrm{KK}^{G}_{\mathrm{ex},\infty}\bigl(\mathbb{C},(A\otimes Cl^{0,1})_{u}\bigr)\xrightarrow{\simeq}\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u}\oplus A_{u})
→≃KKex,∞G​(ℂ,Au)⊕KKex,∞G​(ℂ,Au).\displaystyle\xrightarrow{\simeq}\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u})\oplus\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u}).

It can be directly checked that this composite is the diagonal map of K​Kex,∞G​(ℂ,Au)KK_{\operatorname{ex},\infty}^{G}(\mathbb{C},A_{u}). Since the diagonal map of any spectrum has two canonical retractions, we are done. ∎

Remark 5.5.

At this stage, the reader may want to see an example where the fiber sequence in Equation 5.1 does not split. This is intimately related to a folklore question (Section 5.1), and we discuss it in Section 5.1.

One next want to analyze the fiber sequence in Equation 5.1 when AA is not inner graded. To that end, we give an explicit description of the maps in the sequence at level of π0\pi_{0}.

Lemma 5.5.

Let (A,α)(A,\alpha) be a unital algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. We have a natural group homomorphism

FA:K0G2​(A)→K0G,Fr​(A)F_{A}:K_{0}^{G_{2}}(A)\rightarrow{K}_{0}^{G,\operatorname{Fr}}(A)

given by taking a finitely generated G2G_{2}-equivariant projective AA-module MM to the Fredholm cycle (M,0)∈K0G,Fr​(A)(M,0)\in K_{0}^{G,\operatorname{Fr}}(A).

Proof.

The assertion is clear, modulo the verification that every finitely generated G2G_{2}-equivariant projective AA-module is canonically a graded GG-equivariant Hilbert AA-module. This follows by an easy case by case analysis with signs in light of [8, Proposition 11.2.3]. ∎

Corollary 5.5.

Following the notation of Section 5.1, the diagram

π0​KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\pi_{0}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}π0​KKex,∞G2​(𝒮,A){\lx@inpgf@ignorespaces{\pi_{0}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathcal{S},A)}}K0G2​(A){\lx@inpgf@ignorespaces{K_{0}^{G_{2}}(A)}}K^0G,Fr​(A){\lx@inpgf@ignorespaces{\hat{K}_{0}^{G,\operatorname{Fr}}(A)}}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}^{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}FA\scriptstyle{\lx@inpgf@ignorespaces F_{A}}

commutes.

Proof.

Given a G2G_{2}-equivariant projective AA-module MM, we study the fate of [M]∈K0G2​(A)[M]\in K_{0}^{G_{2}}(A) along the up-right-down itinerary.

The classifying map of MM is a G2G_{2}-equivariant ∗*-homomorphism

φ:ℂ→𝒦A​(V⊗A),\varphi:\mathbb{C}\rightarrow\mathcal{K}_{A}(V\otimes A),

where VV is a finite dimensional G2G_{2}-vector space. φ\varphi is the image of [M][M] in π0​(K​Kex,∞G2​(ℂ,A))\pi_{0}(KK_{\operatorname{ex},\infty}^{G_{2}}(\mathbb{C},A)) under the left vertical map, as can be seen by unraveling the maps in Theorem 3.15 and the equivariant Kasparov stabilization theorem. Also note that 𝒦A​(V⊗A)=ℬA​(V⊗A)\mathcal{K}_{A}(V\otimes A)=\mathcal{B}_{A}(V\otimes A) since 𝒦A​(V⊗A)\mathcal{K}_{A}(V\otimes A) is unital, see [62, Theorem 15.4.2]. It remains to determine the image of φ∘ev0\operatorname{\varphi\circ ev_{0}} under the right vertical map. From Theorem 2.3.5, one gets that this image is the Fredholm cycle (we are also using the notation of the proof of Theorem 2.3.5)

(φ∘ev0⁡(𝒮)​(V⊗A)¯,φ~​(x))=(M,0)(\overline{\varphi\circ\operatorname{ev}_{0}(\mathcal{S})(V\otimes A)},\tilde{\varphi}(x))=(M,0)

Indeed, this follows from the commutative diagram

𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}𝒦A​(φ∘ev0⁡(𝒮)​(V⊗A)¯){\lx@inpgf@ignorespaces{\mathcal{K}_{A}(\overline{\varphi\circ\operatorname{ev}_{0}(\mathcal{S})(V\otimes A)})}}𝒦A​(V⊗A){\lx@inpgf@ignorespaces{\mathcal{K}_{A}(V\otimes A)}}C⁡[−1,1]{\lx@inpgf@ignorespaces{C[-1,1]}}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}(φ∘ev0)nd\scriptstyle{\lx@inpgf@ignorespaces(\varphi\circ\operatorname{ev}_{0})^{\operatorname{nd}}}ev0\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}}ι\scriptstyle{\lx@inpgf@ignorespaces\iota}∃!\scriptstyle{\lx@inpgf@ignorespaces\exists!}ev0\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev}_{0}}φnd\scriptstyle{\lx@inpgf@ignorespaces\varphi^{\operatorname{nd}}}φ\scriptstyle{\lx@inpgf@ignorespaces\varphi}

The dotted extension of (φ∘ev0)nd(\varphi\circ\operatorname{ev}_{0})^{\operatorname{nd}} is unique. However, φnd∘ev0\varphi^{\operatorname{nd}}\circ\operatorname{ev}_{0} is yet another extension, whence they must agree. Our thesis is deduced readily from the latter. ∎

Before stating the next result, we need to setup some notation

Notation 5.5.

Let (A,α)∈𝖦2​𝖢∗​𝖠𝗅𝗀(A,\alpha)\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. Denote by AαA_{\alpha} the GG-equivariant AuA_{u}-module A¯\underline{A} (the underlying abelian group of AA) with the AuA_{u}-action given by a¯.b:=a​α​(b)¯\underline{a}.b:=\underline{a\alpha(b)} and the GG-action given by g.a¯:=g​a¯g.\underline{a}:=\underline{ga}. Note that AαA_{\alpha} is a AuA_{u}-AuA_{u} bimodule in a canonical way.

Lemma 5.5.

Let (A,α)(A,\alpha) be a unital algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. We have a natural group homomorphism

GA:K0G​(Au)→K0G2​(A)G_{A}:K_{0}^{G}(A_{u})\rightarrow K_{0}^{G_{2}}(A)

given by taking a finitely generated GG-equivariant projective AuA_{u}-module MM to the G2G_{2}-equivariant finitely generated projective AA-module M⊕MαM\oplus M_{\alpha}, where Mα:=M⊗AuAαM_{\alpha}:=M\otimes_{A_{u}}A_{\alpha}3333 33 explicitly, MαM_{\alpha} is the abelian group M¯\underline{M} with the AuA_{u}-action given by m¯.a:=m​α​(a)¯\underline{m}.a:=\underline{m\alpha(a)}. MM and MαM_{\alpha} are not isomorphic as AuA_{u}-modules in general. and the C2C_{2}-action on M⊕MτM\oplus M_{\tau} is flip, i.e. given by (m,n¯)↦(n,m¯)(m,\underline{n})\mapsto(n,\underline{m}).

Proof.

Obvious. ∎

Corollary 5.5.

Following the notation of Section 5.1, the diagram

π0​KKex,∞G2​(C​l0,1,A){\lx@inpgf@ignorespaces{\pi_{0}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A)}}π0​KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\pi_{0}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}K0G​(Au){\lx@inpgf@ignorespaces{K_{0}^{G}(A_{u})}}K0G2​(A){\lx@inpgf@ignorespaces{K_{0}^{G_{2}}(A)}}ι∗\scriptstyle{\lx@inpgf@ignorespaces\iota^{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}GA\scriptstyle{\lx@inpgf@ignorespaces G_{A}}

commutes.

Proof.

This follows by chasing through the maps in the diagram. Given a GG-equivariant finitely generated projective AuA_{u}-module MM, the classifying map of [M]∈K0​(Au)[M]\in K_{0}(A_{u}) is a GG-equivariant ∗*-homomorphism

p:ℂ→𝒦Au​(V⊗Au)p:\mathbb{C}\rightarrow\mathcal{K}_{A_{u}}(V\otimes A_{u})

where VV is some finite dimensional GG-vector space. We therefore obtain

indGG2​ℂ→indGG2​pindGG2⁡(𝒦Au​(V⊗Au))↪𝒦A​(V⊗Au⊕V⊗Au,twisted​flip),\operatorname{ind}^{G_{2}}_{G}\mathbb{C}\xrightarrow{\operatorname{ind}^{G_{2}}_{G}p}\operatorname{ind}^{G_{2}}_{G}(\mathcal{K}_{A_{u}}(V\otimes A_{u}))\hookrightarrow\mathcal{K}_{A}(V\otimes A_{u}\oplus V\otimes A_{u},\operatorname{twisted\penalty\ flip}),

where for the last inclusion we used elementary properties of induction for group representations on vector spaces and C∗C^{*}-algebras (see [13, Lemma 4.10]), as well as the description of the co-unit of the induction-restriction adjunction. Precomposing with the inclusion ℂ→indGG2​ℂ\mathbb{C}\rightarrow\operatorname{ind}^{G_{2}}_{G}\mathbb{C}, we conclude that the up-right-down itinerary maps pp to the homomorphism

p~:ℂ→𝒦A​(V⊗Au⊕V⊗Au,twisted​flip),p~​(1)=(p⁡(1)⊕α∗​p​(1)).\tilde{p}:\mathbb{C}\rightarrow\mathcal{K}_{A}(V\otimes A_{u}\oplus V\otimes A_{u},\operatorname{twisted\penalty\ flip}),\penalty\ \penalty\ \penalty\ \penalty\ \tilde{p}(1)=(p(1)\oplus\alpha_{*}p(1)).

It remains to check that the G2G_{2}-equivariant AA-modules (p⁡(1)​(V⊗Au)⊕α∗​p​(1)​(V⊗Au),twisted​flip)(p(1)(V\otimes A_{u})\oplus\alpha_{*}p(1)(V\otimes A_{u}),\operatorname{twisted\penalty\ flip})\penalty\ and (M⊕Mα,flip)(M\oplus M_{\alpha},\operatorname{flip}) are isomorphic. We have p⁡(1)​(V⊗Au)≅Mp(1)(V\otimes A_{u})\cong M as GG-equivariant AuA_{u}-modules by definition. To see that α∗​p​(1)​(V⊗Au)≅Mα\alpha_{*}p(1)(V\otimes A_{u})\cong M_{\alpha} as GG-equivariant AuA_{u}-modules, note that we have

α∗​p​(1)​(V⊗Au)={v⊗α​a∣v⊗a∈p⁡(1)​(V⊗Au)}.\alpha_{*}p(1)(V\otimes A_{u})=\{v\otimes\alpha a\mid v\otimes a\in p(1)(V\otimes A_{u})\}.

The map

φ:(p⁡(1)​(V⊗Au))α\displaystyle\varphi:(p(1)(V\otimes A_{u}))_{\alpha} →α∗​p​(1)​(V⊗Au)\displaystyle\rightarrow\alpha_{*}p(1)(V\otimes A_{u})
v⊗a¯\displaystyle\underline{v\otimes a} ↦v⊗α⁡(a)\displaystyle\mapsto v\otimes\alpha(a)

now readily produces an isomorphism between the GG-equivariant AuA_{u}-modules MαM_{\alpha} and α∗​p​(1)​(V⊗Au)\alpha_{*}p(1)(V\otimes A_{u}). It is now also direct to check that juxtaposing the two isomorphisms yields a G2G_{2}-equivariant isomorphism between (M⊕Mα,flip)(M\oplus M_{\alpha},\operatorname{flip}) and (p⁡(1)​(V⊗Au)⊕α∗​p​(1)​(V⊗Au),twisted​flip).(p(1)(V\otimes A_{u})\oplus\alpha_{*}p(1)(V\otimes A_{u}),\operatorname{twisted\penalty\ flip}). ∎

We end this subsection with the following remark, which connects our results to the classical result of Atiyah-Bott-Shapiro as mentioned in Theorem 1.2. For simplicity, we ignore the external group GG in this remark.

Remark 5.5.

When A=C​ln,0A=Cl^{n,0}, Atiyah-Bott-Shapiro asserts that there are short exact sequences of abelian groups

0→K0C2​(C​ln+1,0)→(C​ln,0→C​ln+1,0)∗K0C2​(C​ln,0)→K^0​(C​ln,0)→0,0\rightarrow K_{0}^{C_{2}}(Cl^{n+1,0})\xrightarrow{(Cl^{n,0}\rightarrow Cl^{n+1,0})^{*}}K_{0}^{C_{2}}(Cl^{n,0})\rightarrow\hat{K}_{0}(Cl^{n,0})\rightarrow 0, (5.6)

where the first map is as described in Section 5.1. Since K^0​(C​ln,0)≅Kn​(ℂ)\hat{K}_{0}(Cl^{n,0})\cong K_{n}(\mathbb{C}), one obtains a convenient (and perhaps miraculous!) description of higher KK-groups of a point as certain Clifford module quotients. This immediately makes one ask the following question.

Question 5.6.

Can the higher KK-groups of any (graded), (Real) unital C∗C^{*}-algebra AA be expressed in terms of Clifford module quotients a’la Atiyah-Bott-Shapiro? More precisely, does there exist a short exact sequence of abelian groups of the form

0→K0C2​(A​⊗^​C​ln+1,0)→(A​⊗^​C​ln,0→A​⊗^​C​ln+1,0)∗K0C2​(A​⊗^​C​ln,0)→K^n​(A)→0?0\rightarrow K_{0}^{C_{2}}(A\hat{\otimes}Cl^{n+1,0})\xrightarrow{(A\hat{\otimes}Cl^{n,0}\rightarrow A\hat{\otimes}Cl^{n+1,0})^{*}}K_{0}^{C_{2}}(A\hat{\otimes}Cl^{n,0})\rightarrow\hat{K}_{n}(A)\rightarrow 0\penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ \penalty\ ?

We explain that the answer to this question is in the negative. To that end, we recall that to show exactness of Equation 5.6 at K^0​(C​ln,0)\hat{K}_{0}(Cl^{n,0}), one explicitly constructs a section of the map K0C2​(C​ln,0)→K^0​(C​ln,0)K_{0}^{C_{2}}(Cl^{n,0})\rightarrow\hat{K}_{0}(Cl^{n,0}) using the notion of index of a Fredholm operator on a Hilbert space with Clifford symmetries. The construction of this index map crucially needs the analytic fact that the kernel of a Fredholm operator on a Hilbert space is automatically finitely generated projective. Since the same is not true for a general Hilbert module over a C∗C^{*}-algebra, the index of a Fredholm operator over an ungraded unital C∗C^{*}-algebra BB is typically defined using the notion of taming (as described in detail in [26, Section 8.2]). Roughly speaking, taming works by adding a dummy finite dimensional free BB-module to the game, and then subtracting it later in the group K0​(B)K_{0}(B). When BB is graded, the taming construction can fail; for example when B:=A​⊗^​C​ln,0B:=A\hat{\otimes}Cl^{n,0} the taming construction can be seen to not necessarily preserve the relevant Clifford symmetries. So in general, one cannot expect to construct the crucial index map witnessing a section of the map K0C2​(A​⊗^​C​ln,0)→K^0​(A​⊗^​C​ln,0)K_{0}^{C_{2}}(A\hat{\otimes}Cl^{n,0})\rightarrow\hat{K}_{0}(A\hat{\otimes}Cl^{n,0}).

And indeed, concrete counterexamples exist. Taking AA to be the complex C∗C^{*}-algebra C⁡(S1,ℂ)C(S^{1},\mathbb{C}) and n=1n=1, we know that K^1​(C⁡(S1,ℂ))≅K1​(C⁡(S1,ℂ))≅ℤ\hat{K}_{1}(C(S^{1},\mathbb{C}))\cong K_{1}(C(S^{1},\mathbb{C}))\cong\mathbb{Z}, but the relevant Clifford module quotient can be shown to be 00. In context of the fiber sequence in Equation 5.5, this failure can be explained to be due to the corresponding boundary map being injective. More elaborations on this can be found in [3, Example 4.51]. See also [10, Appendix A] for other examples and discussions.

5.2 The dual fiber sequence and endomorphisms of KK-groups

In this subsection, we obtain a dual of the fiber sequence described in Section 5.1. The key to the existence of this fiber sequence is the equivalence between C​l1,0Cl^{1,0} and C0​(ℝ0,1)C_{0}(\mathbb{R}^{0,1}) in KKG2!,∞\mathrm{KK}^{G_{2}}_{!,\infty}, as shown in Section 4.1.

Proposition 5.6.

We have a fiber sequence

C​l1,0→𝑗ℂ→𝑝𝒮Cl^{1,0}\xrightarrow{j}\mathbb{C}\xrightarrow{p}\mathcal{S}

in KKex,∞G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}, where j:C​l1,0→ℂj:Cl^{1,0}\rightarrow\mathbb{C} is obtained from the zig-zag C​l1,0→C​l1,1←ℂ,Cl^{1,0}\rightarrow Cl^{1,1}\leftarrow\mathbb{C}, and p∈π0​(KKex,∞G2​(ℂ,𝒮))p\in\pi_{0}(\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},\mathcal{S})) is the image under the resG2C2\operatorname{res}^{C_{2}}_{G_{2}} homomorphism of a generator of K0C2​(𝒮)≅ℤK_{0}^{C_{2}}(\mathcal{S})\cong\mathbb{Z} (Section 2.1).

Proof.

We begin the proof by mentioning that the assertion of the proposition is indeed just: in any stable ∞\infty-category 𝒞\mathcal{C}, a fiber sequence A→𝑓B→𝑔CA\xrightarrow{f}B\xrightarrow{g}C naturally yields a equivalent fiber sequence A→𝑓B→−gCA\xrightarrow{f}B\xrightarrow{-g}C. In light of Section 5.2, it suffices to demonstrate the existence of the fiber sequence in KKex,∞C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty}.

We begin by applying the functor −⊗^​C​l1,0-\hat{\otimes}Cl^{1,0} to Equation 3.2, thereby obtaining the fiber sequence

𝒮​⊗^​C​l1,0→ev0∗C​l1,0→ι∗C​l1,1.\mathcal{S}\hat{\otimes}Cl^{1,0}\xrightarrow{\operatorname{ev}_{0}{{}_{*}}}Cl^{1,0}\xrightarrow{\operatorname{\iota}_{*}}Cl^{1,1}.

Now, Section 4 and Section 4.1 show that we have a fiber sequence

Ω​𝒮→C​l1,0→ι∗C​l1,1\Omega\mathcal{S}\rightarrow Cl^{1,0}\xrightarrow{\iota_{*}}Cl^{1,1}

in KKex,∞C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty}. Taking cofibering in KKex,∞C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty} and using the equivalence ℂ≃C​l1,1\mathbb{C}\simeq Cl^{1,1} we obtain a fiber sequence

C​l1,0→𝑗ℂ→𝒮.Cl^{1,0}\xrightarrow{j}\mathbb{C}\rightarrow\mathcal{S}.

To prove our thesis, it will suffice to show that the second morphism above is a generator of K0C2​(𝒮)≅ℤK_{0}^{C_{2}}(\mathcal{S})\cong\mathbb{Z}. Consider the long exact sequence of K∗C2​(−)(=π∗​KKex,∞C2​(ℂ,−))K_{*}^{C_{2}}(-)(=\pi_{*}\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty}(\mathbb{C},-)) groups associated to this fiber sequence

...→K0C2(Cl1,0)→j∗K0C2(ℂ)→K0C2(𝒮)→∂K−1C2(Cl1,0)→…...\rightarrow K_{0}^{C_{2}}(Cl^{1,0})\xrightarrow{j_{*}}K_{0}^{C_{2}}(\mathbb{C})\rightarrow K_{0}^{C_{2}}(\mathcal{S})\xrightarrow{\partial}K_{-1}^{C_{2}}(Cl^{1,0})\rightarrow...

By tensor invertibility of C​l0,1Cl^{0,1} in KKex,∞C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty} and the induction-restriction adjunction, we have

K−1C2​(C​l1,0)≅K−1​(ℂu)≅0,K_{-1}^{C_{2}}(Cl^{1,0})\cong K_{-1}(\mathbb{C}_{u})\cong 0,

whence the map

K0C2​(ℂ)→K0C2​(𝒮)K_{0}^{C_{2}}(\mathbb{C})\rightarrow K_{0}^{C_{2}}(\mathcal{S})

above is surjective. We now consider the square

K0C2​(ℂ){\lx@inpgf@ignorespaces{K_{0}^{C_{2}}(\mathbb{C})}}K0C2​(𝒮){\lx@inpgf@ignorespaces{K_{0}^{C_{2}}(\mathcal{S})}}ℤ⊕ℤ{\lx@inpgf@ignorespaces{\mathbb{Z}\oplus\mathbb{Z}}}ℤ,{\lx@inpgf@ignorespaces{\mathbb{Z}},}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}†\scriptstyle{\lx@inpgf@ignorespaces{\dagger}}

where the vertical maps are isomorphisms as mentioned in Section 2.1 and Section 2.1, and the map †\dagger is so defined to make the diagram commute. Now, since the morphisms in the square are also C2C_{2}-equivariant and the C2C_{2}-abelian group ℤ⊕ℤ\mathbb{Z}\oplus\mathbb{Z} is generated by (1,0)(1,0), we conclude from the surjectivity of †{\dagger} that it maps (1,0)(1,0) to ±1\pm 1. ∎

Proposition 5.6.

We have a natural fiber sequence

𝕂^G​(A)→𝕂G2​(A)→𝕂G​((A​⊗^​C​l0,2)u)\hat{\mathbb{K}}^{G}(A)\xrightarrow{}\mathbb{K}^{G_{2}}(A)\xrightarrow{}\mathbb{K}^{G}((A\hat{\otimes}Cl^{0,2})_{u}) (5.7)

for every A∈𝖦2​𝖢∗​𝖠𝗅𝗀A\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}.

Proof.

We apply the exact functor

KKex,∞G2​(−,A):𝖦2​𝖢∗​𝖠𝗅𝗀⟶Sp.\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(-,A):\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}\longrightarrow\operatorname{Sp}.

to the fiber sequence in Section 5.2. In light of the proof of Section 5.1, we only need to identify KKex,∞G2​(C​l1,0,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A) with 𝕂G​((A​⊗^​C​l0,2)u)\mathbb{K}^{G}((A\hat{\otimes}Cl^{0,2})_{u}). For that we use the route

KKex,∞G2​(C​l1,0,A)→≃−⊗^​C​l0,2KKex,∞G2​(C​l1,2,A​⊗^​C​l0,2)→≃(C​l0,1→C​l1,2)∗KKex,∞G2​(C​l0,1,A​⊗^​C​l0,2)→≃𝗂𝗇𝖽⊣𝗋𝖾𝗌𝕂G​((A​⊗^​C​l0,2)u).\resizebox{22609920}{}{$\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)\xrightarrow[\simeq]{-\hat{\otimes}Cl^{0,2}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,2},A\hat{\otimes}Cl^{0,2})\xrightarrow[\simeq]{(Cl^{0,1}\rightarrow Cl^{1,2})^{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A\hat{\otimes}Cl^{0,2})\xrightarrow[\simeq]{\mathsf{ind}\dashv\mathsf{res}}\mathbb{K}^{G}\bigl((A\hat{\otimes}Cl^{0,2})_{u}\bigr)$}.

∎

At this juncture, we record an interpretation of the map j∗:KKex,∞G2​(ℂ,A)→KKex,∞G2​(C​l1,0,A)j^{*}:\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)\rightarrow\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A) which will come handy later.

Lemma 5.7.

The diagram

KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(C​l1,0,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)}}KKex,∞G2​(C​l1,1,A​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,1},A\hat{\otimes}Cl^{0,1})}}KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(ℂ,A​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A\hat{\otimes}Cl^{0,1})}}j∗\scriptstyle{\lx@inpgf@ignorespaces j^{*}}=\scriptstyle{\lx@inpgf@ignorespaces=}⊗^​C​l0,1,≃\scriptstyle{\lx@inpgf@ignorespaces\hat{\otimes}Cl^{0,1},\,\simeq}(ℂ→C​l1,1)∗,≃\scriptstyle{\lx@inpgf@ignorespaces(\mathbb{C}\rightarrow Cl^{1,1})_{*},\,\simeq}(A→A​⊗^​C​l0,1)∗\scriptstyle{\lx@inpgf@ignorespaces(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}}

commutes.

Proof.

We expand the diagram to

KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(C​l1,0,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)}}KKex,∞G2​(C​l1,1,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,1},A)}}KKex,∞G2​(C​l1,1,A​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,1},A\hat{\otimes}Cl^{0,1})}}KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(ℂ,A​⊗^​C​l0,1){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A\hat{\otimes}Cl^{0,1})}}j∗\scriptstyle{\lx@inpgf@ignorespaces j^{*}}=\scriptstyle{\lx@inpgf@ignorespaces=}⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces\hat{\otimes}Cl^{0,1}}(ℂ→C​l1,1)∗\scriptstyle{\lx@inpgf@ignorespaces(\mathbb{C}\rightarrow Cl^{1,1})^{*}}(C​l1,0→C​l1,1)∗\scriptstyle{\lx@inpgf@ignorespaces(Cl^{1,0}\rightarrow Cl^{1,1})^{*}}(A→A​⊗^​C​l0,1)∗\scriptstyle{\lx@inpgf@ignorespaces(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}}(ℂ→C​l1,1)∗\scriptstyle{\lx@inpgf@ignorespaces(\mathbb{C}\rightarrow Cl^{1,1})^{*}}(ℂ→C​l1,1)∗\scriptstyle{\lx@inpgf@ignorespaces(\mathbb{C}\rightarrow Cl^{1,1})^{*}}(A→A​⊗^​C​l0,1)∗\scriptstyle{\lx@inpgf@ignorespaces(A\rightarrow A\hat{\otimes}Cl^{0,1})_{*}}

It suffices to show that each of the four shapes with one vertex KKex,∞G2​(C​l1,1,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,1},A) commutes. But all of them are clear (for the right-angled triangle shaped diagram, use an argument similar to the one for Equation 5.4). ∎

Unlike in the case of Section 5.1, the induced maps at the level of π0\pi_{0} groups of the fiber sequence in Equation 5.7 are not easy to write down explicitly. We instead discuss the various endomorphisms of the KK-theory groups that arise from the fiber sequences in Equation 5.1 and Equation 5.7.

Consider the following diagram in KKex,∞C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},\infty}:

C​l1,0{\lx@inpgf@ignorespaces{Cl^{1,0}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}ℂ{\lx@inpgf@ignorespaces{\mathbb{C}}}C​l0,1{\lx@inpgf@ignorespaces{Cl^{0,1}}}𝒮{\lx@inpgf@ignorespaces{\mathcal{S}}}j\scriptstyle{\lx@inpgf@ignorespaces j}ev0\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev_{0}}}ι\scriptstyle{\lx@inpgf@ignorespaces\iota}p\scriptstyle{\lx@inpgf@ignorespaces p}
Lemma 5.7.

ev0∘p=1−x∈KKex,0C2​(ℂ,ℂ)≅Z⁡[x]x2=1\operatorname{ev}_{0}\circ p=1-x\in\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C})\cong\frac{Z[x]}{x^{2}=1}, with the isomorphism being as in Section 2.1.1 (keeping in mind Theorem 3.153434 34 the two natural ring structures on the endomorphisms of the unit in any monoidal category coincide thanks to the Eckmann-Hilton argument. See also [14, Lemma 5.1].).

Proof.

From Section 2.1 and Section 2.1, we have a short exact sequence

0→K0C2​(𝒮)→ev0∗K0C2​(ℂ)→ι∗K0C2​(C​l0,1)→0.0\rightarrow K_{0}^{C_{2}}(\mathcal{S})\xrightarrow{{\operatorname{ev}_{0}}_{*}}K_{0}^{C_{2}}(\mathbb{C})\xrightarrow{\iota_{*}}K_{0}^{C_{2}}(Cl^{0,1})\rightarrow 0.

The composition in the KKex,0C2\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}-category will be the image of pp under ev0∗\operatorname{ev_{0_{*}}}. The rest follows from Section 2.1. ∎

We now record a corollary of the above calculation which will come handy later.

Corollary 5.7.

The diagram

KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}(ev0∘p)∗\scriptstyle{\lx@inpgf@ignorespaces(\operatorname{ev}_{0}\circ p)_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}n↦2​n\scriptstyle{\lx@inpgf@ignorespaces n\mapsto 2n}

commutes.

Proof.

It suffices to show that the diagram commutes on [ev0][\operatorname{ev}_{0}]. The bottom-right itinerary maps it to 2∈ℤ2\in\mathbb{Z}. To analyse its fate under the right-down itinerary, we bring Section 5.2 into play, which shows that the upper horizontal arrow is product in KKC2!,∞\mathrm{KK}^{C_{2}}_{!,\infty}-product with ([ℂtriv]−[ℂsign])([\mathbb{C}^{\operatorname{triv}}]-[\mathbb{C}^{\operatorname{sign}}]).

Postcomposition with [ℂ]triv[\mathbb{C}]^{\operatorname{triv}} maps [ev0][\operatorname{ev}_{0}] to itself, since [ℂtriv][\mathbb{C}^{\operatorname{triv}}] is the identity element of KKex,0C2​(ℂ,ℂ)\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C}). To prove our thesis, we have to show that postcomposition with [ℂsign][\mathbb{C}^{\operatorname{sign}}] maps [ev0][\operatorname{ev}_{0}] to −[ev0]-[\operatorname{ev}_{0}]. Unraveling the definition of postcomposition with [ℂsign][\mathbb{C}^{\operatorname{sign}}], this follows directly from the proof of Theorem 2.3.1. ∎

Corollary 5.7.

Let AA be a unital algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. The composite

K0G2​(A)→ev0∗K^0G​(A)→p∗K0G2​(A)K_{0}^{G_{2}}(A)\xrightarrow{\operatorname{ev}_{0}^{*}}\hat{K}^{G}_{0}(A)\xrightarrow{p^{*}}K^{G_{2}}_{0}(A)

maps a finitely generated G2G_{2}-equivariant projective AA-module MM to [M]−[Mop]∈K0G2​(A)[M]-[M^{\operatorname{op}}]\in K_{0}^{G_{2}}(A), where MopM^{\operatorname{op}} is MM as a GG-equivariant AuA_{u}-module, with the C2C_{2}-action given as the negative of the C2C_{2}-action on MM.

Proof.

Unraveling the definitions and from Section 5.2, we conclude that the composite is nothing but the composition with the image under resG2C2\operatorname{res}^{C_{2}}_{G_{2}} of 1−x∈KKex,0G2​(ℂ,ℂ)≅Z⁡[x]x2=11-x\in\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C})\cong\frac{Z[x]}{x^{2}=1}. Identifying KKex,0G2​(ℂ,ℂ)\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C}) with the classical G2G_{2}-equivariant KK-theory of a point, it is clear that 11 corresponds to the trivial representation, and xx corresponds to the sign representation of G2G_{2} on ℂ\mathbb{C}.3535 35 more precisely, GG acts trivially on ℂ\mathbb{C} in both cases, and C2C_{2} acts either trivially or via the sign representation. Since the internal and external products

KKex,0G2​(ℂ,ℂ)×KKex,0G2​(ℂ,A)→KKex,0G2​(ℂ,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C})\times\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},A)\rightarrow\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},A)

are the same (this is true in any monoidal category), our thesis follows since the external multiplication of [M][M] with xx yields [Mop][M^{\operatorname{op}}] (keeping in mind the lax monoidality assertion of Theorem 3.15). ∎

The proof of the next result requires slightly more work than needed in the proof of Section 5.2, but is similar in spirit. Somewhat surprisingly Section 5.2 is needed in the proof!

Lemma 5.7.

p∘ev0=1+x∈KKex,0G2​(𝒮,𝒮)≅Z⁡[x]x2=1p\circ\operatorname{ev}_{0}=1+x\in\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathcal{S})\cong\frac{Z[x]}{x^{2}=1}, with the isomorphism being as in Section 3.7.

Proof.

From the fiber sequence of Section 5.2, we obtain a long exact sequence of K^∗​(−)(=KKex,0G2​(𝒮,−))\hat{K}_{*}(-)(=\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathcal{S},-)) groups

⋯⟶K^0​(C​l1,0)→j∗K^0​(ℂ)→p∗K^0​(𝒮)→∂⋯\cdots\longrightarrow\hat{K}_{0}(Cl^{1,0})\xrightarrow{j_{*}}\hat{K}_{0}(\mathbb{C})\xrightarrow{p_{*}}\hat{K}_{0}(\mathcal{S})\xrightarrow{\partial}\cdots

The composition p∘ev0p\circ\operatorname{ev}_{0} will be the image of [ev0][\operatorname{ev}_{0}] under p∗p_{*}. Since p∗p_{*} is a C2C_{2}-equivariant map, there exists k∈ℤk\in\mathbb{Z} rendering the diagram

K^0​(ℂ){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathbb{C})}}K^0​(𝒮){\lx@inpgf@ignorespaces{\hat{K}_{0}(\mathcal{S})}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}ℤ⊕ℤ{\lx@inpgf@ignorespaces{\mathbb{Z}\oplus\mathbb{Z}}}p∗\scriptstyle{\lx@inpgf@ignorespaces p_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}1↦(k,k)\scriptstyle{\lx@inpgf@ignorespaces 1\mapsto(k,k)} (5.8)

commutative, where the left isomorphism is the standard one (mapping [ev0][\operatorname{ev}_{0}] to 11), and the right one is the one mentioned in Section 2.2.8.

Claim.

k=1k=1 in the above diagram.

Proof.

We expand the diagram to

KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}KKex,0C2​(𝒮,𝒮){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathcal{S})}}KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}ℤ⊕ℤ{\lx@inpgf@ignorespaces{\mathbb{Z}\oplus\mathbb{Z}}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}p∗\scriptstyle{\lx@inpgf@ignorespaces p_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}ev0∗\scriptstyle{\lx@inpgf@ignorespaces\operatorname{ev_{0}}_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}(n,m)↦n+m\scriptstyle{\lx@inpgf@ignorespaces(n,m)\mapsto n+m} (5.9)

Observe that the right square commutes, as can be explicitly checked on the two generators [id𝒮][\operatorname{id_{\mathcal{S}}}] and [α𝒮][\alpha_{\mathcal{S}}]. Furthermore, the rectangle

KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}KKex,0C2​(𝒮,ℂ){\lx@inpgf@ignorespaces{\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathcal{S},\mathbb{C})}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}ℤ{\lx@inpgf@ignorespaces\mathbb{Z}}(ev0∘p)∗\scriptstyle{\lx@inpgf@ignorespaces(\operatorname{ev}_{0}\circ p)_{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}n↦2​n\scriptstyle{\lx@inpgf@ignorespaces n\mapsto 2n}

commutes too, as seen in Section 5.2. The claim follows. ∎

This also finishes the proof of the lemma. ∎

Corollary 5.9.

Let AA be a unital algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. The composite

K0G,Fr​(A)→p∗K0G2​(A)→ev0∗K0G,Fr​(A){K}_{0}^{G,\operatorname{Fr}}(A)\xrightarrow{p^{*}}K_{0}^{G_{2}}(A)\xrightarrow{\operatorname{ev}_{0}^{*}}{K}^{G,\operatorname{Fr}}_{0}(A)

maps the Fredholm cycle (ℰ,F)∈K0G,Fr​(A)(\mathcal{E},F)\in{K}_{0}^{G,\operatorname{Fr}}(A) to (ℰ⊕ℰ,F⊕(−F))∈K0G,Fr​(A)(\mathcal{E}\oplus\mathcal{E},F\oplus(-F))\in{K}_{0}^{G,\operatorname{Fr}}(A).

Proof.

This follows from Section 5.2 and the formula of the explicit isomorphism π0​𝕂G,sp​(A)≅K0G,Fr​(A)\pi_{0}{\mathbb{K}}^{\operatorname{G,sp}}(A)\cong{K}_{0}^{G,\operatorname{Fr}}(A) as mentioned in Theorem 2.3.6. ∎

Remark 5.9.

Note that (ℰ,−F)(\mathcal{E},-F) is not the inverse of (ℰ,F)∈K0G,Fr​(A)(\mathcal{E},F)\in{{K}}^{G,\operatorname{Fr}}_{0}(A); the usual formula of the inverse also requires to flip the grading on ℰ\mathcal{E} (see [26, Lemma 8.24] for details). In fact, when AA is inner graded, (ℰ,−F)=(ℰ,F)(\mathcal{E},-F)=(\mathcal{E},F), as can be seen from Theorem 2.3.6. Thus, for inner graded AA, K0G,Fr​(A)→ev0∗∘p∗K0G,Fr​(A){K}_{0}^{G,\operatorname{Fr}}(A)\xrightarrow{\operatorname{ev}_{0}^{*}\circ p^{*}}{K}_{0}^{G,\operatorname{Fr}}(A) is the multiplication by 22 map.

We now consider the composite

𝕂G​(Au)→ι∗𝕂G2​(A)→j∗𝕂G​((A​⊗^​C​l0,2)u).\mathbb{K}^{G}(A_{u})\xrightarrow{\iota^{*}}\mathbb{K}^{G_{2}}(A)\xrightarrow{j^{*}}\mathbb{K}^{G}((A\hat{\otimes}Cl^{0,2})_{u}).

For a general unital A∈𝖦2​𝖢∗​𝖠𝗅𝗀A\in\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. the composite does not have an illuminating description, since we do not have a good understanding of the algebra (A​⊗^​C​l0,2)u(A\hat{\otimes}Cl^{0,2})_{u}. However, the situation is better in the following cases

  1. 1.

    AA is inner graded (and potentially Real).

  2. 2.

    AA is complex (with potentially non-inner grading).

We begin with the first case. So let AA be a unital, inner graded algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. Then, we assert that the map of spectra KKex,∞G2​(ℂ,A)→j∗KKex,∞G2​(C​l1,0,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)\xrightarrow{j^{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A) splits. To see this, we identify KKex,∞G2​(C​l1,0,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A) with 𝕂G​(Au)\mathbb{K}^{G}(A_{u}) via the route:

KKex,∞G2​(C​l1,0,A)→≃−⊗^​C​l0,1KKex,∞G2​(C​l1,1,A​⊗^​C​l0,1)→A​inner graded,≃(ℂ→C​l1,1)∗KKex,∞G2​(ℂ,A⊗C​l0,1)→≃res⊣𝖼𝗈𝗂𝗇𝖽𝕂G​(Au).\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)\xrightarrow[\simeq]{-\hat{\otimes}Cl^{0,1}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,1},A\hat{\otimes}Cl^{0,1})\xrightarrow[A\penalty\ \text{inner graded},\simeq]{(\mathbb{C}\rightarrow Cl^{1,1})^{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A\otimes Cl^{0,1})\xrightarrow[\simeq]{\operatorname{res}\dashv\mathsf{coind}}\mathbb{K}^{G}(A_{u}). (5.10)

We want to understand the induced map 𝕂G2​(A)→𝕂G​(A)\mathbb{K}^{G_{2}}(A)\rightarrow\mathbb{K}^{G}(A) under the identification above. To that end, we need the following lemma.

Lemma 5.10.

The diagram

KKex,∞G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)}}KKex,∞G2​(C​l1,0,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)}}𝕂G2​(A){\lx@inpgf@ignorespaces{\mathbb{K}^{G_{2}}(A)}}𝕂G​(Au){\lx@inpgf@ignorespaces{\mathbb{K}^{G}(A_{u})}}j∗\scriptstyle{\lx@inpgf@ignorespaces j^{*}}≃\scriptstyle{\lx@inpgf@ignorespaces\simeq}≃\scriptstyle{\lx@inpgf@ignorespaces\simeq}𝗋𝖾𝗌GG2​(−)\scriptstyle{\lx@inpgf@ignorespaces\mathsf{res}^{G_{2}}_{G}(-)}

commutes, where the left vertical equivalence is induced from Theorem 3.15, and the right vertical equivalence is induced by Equation 5.10. In particular, for unital AA, the induced map K0G2​(A)→K0G​(A)K_{0}^{G_{2}}(A)\rightarrow K_{0}^{G}(A) forgets the C2C_{2}-action on a G2G_{2}-equivariant projective AA-module in K0G2​(A)K_{0}^{G_{2}}(A).

Proof.

In light of Section 5.2, we just need to show that the composite

KKex,∞G2​(ℂ,A)→(A→A⊗C​l0,1)∗KKex,∞G2​(ℂ,A⊗C​l0,1)→≅res⊣coindKKex,∞G​(ℂ,Au)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A)\xrightarrow{(A\rightarrow A\otimes Cl^{0,1})_{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(\mathbb{C},A\otimes Cl^{0,1})\xrightarrow[\cong]{\text{res}\dashv\text{coind}}\mathrm{KK}^{G}_{\mathrm{ex},\infty}(\mathbb{C},A_{u})

identifies with the restriction map. But this is clear in light of description of the counit of the restriction-coinduction adjunction as mentioned in Theorem 3.13 (the adjunction holds good for non-separable algebras too). ∎

Proposition 5.10.

Let AA be an inner graded algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}. Then, the fiber sequence in Equation 5.7 splits.

Proof.

In light of Section 5.2, it suffices to construct a section of the map 𝕂G2​(A)→𝗋𝖾𝗌GG2​(−)𝕂G​(Au)\mathbb{K}^{G_{2}}(A)\xrightarrow{\mathsf{res}^{G_{2}}_{G}(-)}\mathbb{K}^{G}(A_{u}). If AA were trivially graded, this section could have been taken to be 𝗋𝖾𝗌G2G​(−)\mathsf{res}^{G}_{G_{2}}(-). In the general inner graded case, we use the fact that A≃resG2G​resGG2​AA\simeq\operatorname{res}^{G}_{G_{2}}\operatorname{res}^{G_{2}}_{G}A in KKex,∞G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty} as follows by an application of [63, Example E.2.13] (see also [16, Lemma 2.1]). ∎

As an immediate consequence of Section 5.2, we have the following corollary.

Corollary 5.10.

Let (A,α)(A,\alpha) be a unital, inner graded algebra in 𝖦2​𝖢∗​𝖠𝗅𝗀\mathsf{G}_{2}\mathsf{C}^{*}\!\mathsf{Alg}.

  1. 1.

    The composite K0G​(Au)→ι∗K0G2​(A)→j∗K0G​(Au)K_{0}^{G}(A_{u})\xrightarrow{\iota^{*}}K_{0}^{G_{2}}(A)\xrightarrow{j^{*}}K_{0}^{G}(A_{u}) is given by

    K0G​(Au)\displaystyle K_{0}^{G}(A_{u}) →K0G​(Au)\displaystyle\rightarrow K_{0}^{G}(A_{u})
    [M]\displaystyle[M] ↦[M⊕Mα]=2​[M]\displaystyle\mapsto[M\oplus M_{\alpha}]=2[M]
  2. 2.

    The composite K0G2​(A)→j∗K0G​(Au)→ι∗K0G2​(A)K_{0}^{G_{2}}(A)\xrightarrow{j^{*}}K_{0}^{G}(A_{u})\xrightarrow{\iota^{*}}K_{0}^{G_{2}}(A) is given by

    K0G2​(A)\displaystyle K_{0}^{G_{2}}(A) →K0G2​(A)\displaystyle\rightarrow K_{0}^{G_{2}}(A)
    [M,αM]\displaystyle[M,\alpha_{M}] ↦[M⊕Mα,flip]=[M⊕M,(m,n)↦(αM(n),αM(m))]\displaystyle\mapsto[M\oplus M_{\alpha},\operatorname{flip}]=[M\oplus M,(m,n)\mapsto(\alpha_{M}(n),\alpha_{M}(m))]
Proof.

Everything follows immediately from Section 5.1 and Section 5.2, except that we have to justify the equalities in Assertions 1 and 2.

For Assertion 1, it suffices to show that for MM a GG-equivariant AuA_{u}-module over an inner graded AA, then Mα≅MM_{\alpha}\cong M as GG-equivariant AuA_{u}-modules. If uu is the symmetry implementing the grading on AA, then

Mα→M,m¯↦m​uM_{\alpha}\rightarrow M,\penalty\ \penalty\ \penalty\ \underline{m}\mapsto mu

is such an isomorphism.

For Assertion 2, we first show that when MM is a G2G_{2}-equivariant projective AA-module, then M≅MαM\cong M_{\alpha} as GG-equivariant AuA_{u}-modules. Indeed, an isomorphism is given by

M\displaystyle M →Mα\displaystyle\rightarrow M_{\alpha}
m\displaystyle m ↦αM​(m)¯\displaystyle\mapsto\underline{\alpha_{M}(m)}

Under this isomorphism, [M⊕Mα,flip]=[M⊕M,(m,n)↦(αM(n),αM(m))]∈K0G2(A)[M\oplus M_{\alpha},\operatorname{flip}]=[M\oplus M,(m,n)\mapsto(\alpha_{M}(n),\alpha_{M}(m))]\in K_{0}^{G_{2}}(A). Also compare the proof of Section 5.1.3636 36 actually this argument did not use that AA is inner graded, see also Section 5.2. ∎

We now tackle the case when AA is a (potentially non-inner graded) complex C∗C^{*}-algebra. In this case, we recall that there is a preferred isomorphism C​l1,0≅C​l0,1Cl^{1,0}\cong Cl^{0,1}, mapping the canonical generator of C​l1,0Cl^{1,0} to ii times the canonical generator of C​l0,1Cl^{0,1}. Furthermore, the diagram

C​l1,0{\lx@inpgf@ignorespaces{Cl^{1,0}}}C​l1,1{\lx@inpgf@ignorespaces{Cl^{1,1}}}C​l0,1{\lx@inpgf@ignorespaces{Cl^{0,1}}}−⊗^​C​l0,1\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}Cl^{0,1}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}−⊗^​C​l1,0\scriptstyle{\lx@inpgf@ignorespaces-\hat{\otimes}Cl^{1,0}} (5.11)

commutes up to homotopy, as can be easily constructed via the usual sine-cosine formula. We can therefore identify KKex,∞G2​(C​l1,0,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A) with 𝕂G​(Au)\mathbb{K}^{G}(A_{u}) via the route

KKex,∞G2​(C​l1,0,A)≃KKex,∞G2​(C​l0,1,A)≃𝕂G​(Au),\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{1,0},A)\simeq\mathrm{KK}^{G_{2}}_{\mathrm{ex},\infty}(Cl^{0,1},A)\simeq\mathbb{K}^{G}(A_{u}), (5.12)

where the last equivalence stems from the induction-restriction adjunction.

Lemma 5.12.

The diagram

KKex,0G2​(ℂ,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},A)}}KKex,0G2​(C​l1,0,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(Cl^{1,0},A)}}KKex,0G2​(C​l0,1,A){\lx@inpgf@ignorespaces{\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(Cl^{0,1},A)}}K0G2​(A){\lx@inpgf@ignorespaces{K_{0}^{G_{2}}(A)}}K0G​(Au){\lx@inpgf@ignorespaces{K_{0}^{G}(A_{u})}}j∗\scriptstyle{\lx@inpgf@ignorespaces j^{*}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}forget C2\scriptstyle C_{2} action≅\scriptstyle{\lx@inpgf@ignorespaces\cong}

commutes, where the left vertical isomorphism is induced from Theorem 3.15, and the other maps are as described above.3737 37 we use the same notations as in the Real case; this should not create any confusion.

Proof.

The commutativity of the upper right triangle follows from the commutativity up to homotopy of Equation 5.11. The commutativity of the trapezoid follows from explicitly chasing the definitions, similar to the proof of Section 5.1. ∎

Corollary 5.12.

Let (A,α)(A,\alpha) be a unital, complex G×C2G\times C_{2}-equivariant complex C∗C^{*}-algebra.

  1. 1.

    The composite K0G​(Au)→ι∗K0G2​(A)→j∗K0G​(Au)K_{0}^{G}(A_{u})\xrightarrow{\iota^{*}}K_{0}^{G_{2}}(A)\xrightarrow{j^{*}}K_{0}^{G}(A_{u}) is given by

    K0G​(Au)\displaystyle K_{0}^{G}(A_{u}) →K0G​(Au)\displaystyle\rightarrow K_{0}^{G}(A_{u})
    [M]\displaystyle[M] ↦[M⊕Mα]\displaystyle\mapsto[M\oplus M_{\alpha}]
  2. 2.

    The composite K0G2​(A)→j∗K0G​(Au)→ι∗K0G2​(A)K_{0}^{G_{2}}(A)\xrightarrow{j^{*}}K_{0}^{G}(A_{u})\xrightarrow{\iota^{*}}K_{0}^{G_{2}}(A) is given by

    K0G2​(A)\displaystyle K_{0}^{G_{2}}(A) →K0G2​(A)\displaystyle\rightarrow K_{0}^{G_{2}}(A)
    [M,αM]\displaystyle[M,\alpha_{M}] ↦[M⊕Mα,flip]=[M⊕M,(m,n)↦(αM(n),αM(m))]\displaystyle\mapsto[M\oplus M_{\alpha},\operatorname{flip}]=[M\oplus M,(m,n)\mapsto(\alpha_{M}(n),\alpha_{M}(m))]
Proof.

Exactly the same proof as Section 5.2. ∎

Remark 5.12.

We also mention another description of the map K0G2​(A)→K0G2​(A)K_{0}^{G_{2}}(A)\rightarrow K_{0}^{G_{2}}(A) as in Section 5.2.2. Using the isomorphism C​l1,0≅C​l0,1Cl^{1,0}\cong Cl^{0,1}, we can treat the composition

KKex,0G2​(ℂ,A)→j∗KKex,0G2​(C​l1,0,A)≃KKex,0G2​(C​l0,1,A)→ι∗KKex,0G2​(ℂ,A)\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},A)\xrightarrow{j^{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(Cl^{1,0},A)\simeq\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(Cl^{0,1},A)\xrightarrow{\iota^{*}}\mathrm{KK}^{G_{2}}_{\mathrm{ex},0}(\mathbb{C},A)

as the KKex,0G2\mathrm{KK}^{G_{2}}_{\mathrm{ex},0} product by the image under resG2C2\operatorname{res}^{C_{2}}_{G_{2}} of a certain element in KKex,0C2​(ℂ,ℂ)\mathrm{KK}^{C_{2}}_{\mathrm{ex},0}(\mathbb{C},\mathbb{C}). It turns out that this element is3838 38 we omit the details since it is not really needed anywhere (1,1)(1,1), whence the induced map must be

K0G2​(A)\displaystyle K_{0}^{G_{2}}(A) →K0G2​(A)\displaystyle\rightarrow K_{0}^{G_{2}}(A)
[M,αM]\displaystyle[M,\alpha_{M}] ↦[M⊕Mop,αM⊕(−αM)]\displaystyle\mapsto[M\oplus M^{\operatorname{op}},\alpha_{M}\oplus(-\alpha_{M})]

And indeed, we have an isomorphism of G2G_{2}-equivariant AA-modules

M⊕Mα\displaystyle M\oplus M_{\alpha} →M⊕Mop\displaystyle\rightarrow M\oplus M^{\operatorname{op}}
(m,n¯)\displaystyle(m,\underline{n}) ↦(m+αM​(n)2,m−αM​(n)2).\displaystyle\mapsto(\frac{m+\alpha_{M}(n)}{2},\frac{m-\alpha_{M}(n)}{2}).

Thus, we actually have isomorphisms of G2G_{2}-equivariant AA-modules

(M⊕Mop,αM⊕(−αM))≅(M⊕Mα,flip)≅(M⊕M,(m,n)↦(αM(n),αM(n))).(M\oplus M^{\operatorname{op}},\alpha_{M}\oplus(-\alpha_{M}))\cong(M\oplus M_{\alpha},\operatorname{flip})\cong(M\oplus M,(m,n)\mapsto(\alpha_{M}(n),\alpha_{M}(n))).
Remark 5.12.

Note that when AA is a non-inner graded C∗C^{*}-algebra, the fiber sequence in Equation 5.7 need not split. A concrete counterexample is A=ℂ​l1A=\mathbb{C}l^{1}, since K0C2​(ℂ​l1)≅ℤK_{0}^{C_{2}}(\mathbb{C}l^{1})\cong\mathbb{Z} (Section 2.1) and K0​(ℂ​lu3)≅K0​(ℂ​lu1)≅ℤ⊕ℤK_{0}(\mathbb{C}l^{3}_{u})\cong K_{0}(\mathbb{C}l^{1}_{u})\cong\mathbb{Z}\oplus\mathbb{Z}.

6 Connections with classical bivariant KK-theories

We finally want to show that the homotopy categories of the full subcategories of the graded KK^G!,∞\widehat{\mathrm{KK}}^{G}_{!,\infty} categories spanned by separable algebras can be identified with classical graded (Kasparov’s) K​KGKK^{G} ([39], [40])-category or (Connes-Higson’s) EGE^{G}-category ([20],[29],[32]), according as !=se!=\operatorname{se} or !=ex!=\operatorname{ex}, respectively. We give a self contained treatment for the case of EE-theory; see Section 6.4 for a discussion on the graded K​KKK-theoretic analogue.

As mentioned in the introduction, the results of this section are not relevant for our study of graded/equivariant/classical KK-theory as in Section 5.

6.1 Recapitulation of classical ungraded K​KGKK^{G}-theory

We begin by recalling the classical definitions of the ungraded (Real) K​KGKK^{G}-categories. Kasparov in his seminal work defined them in terms of now-called Kasparov modules: given GG-C∗C^{*}-algebras AA and BB, KKKasG​(A,B)\mathrm{KK}^{G}_{\mathrm{Kas}}(A,B) was built out of certain equivalence classes of triples (ℰ,φ,F)(\mathcal{E},\varphi,F) comprising of a Hilbert GG-BB-module ℰ\mathcal{E}, a equivariant representation φ\varphi of AA on the adjointable operators on ℰ\mathcal{E}, and an adjointable operator FF on ℰ\mathcal{E} satisfying certain compactness and equivariance conditions3939 39 Kasparov worked with graded algebras and modules from the get-go.. It then takes a truckload of work to prove that upon restricting to separable algebras there exists a composition law, now known as the Kasparov product

KKKasG,sep​(A,B)×KKKasG,sep​(B,C)→KKKasG,sep​(A,C)\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}(A,B)\times\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}(B,C)\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}(A,C)

which is unital and associative, and one concludes that KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} is a category.

Since every equivariant ∗*-homomorphism naturally gives a Kasparov module, we have a canonical functor

kkKasG,sep:𝖦𝖢∗​𝖠𝗅𝗀sep→KKKasG,sep.\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}.

The question whether the category KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} has a universal property was settled in [58, Theorem 2.2],[46, Theorem 6.6] (with non-equivariantly the issue being first tackled in [33, Theorem 4.5]). Note that Meyer also mentions (as can be readily checked too) that the results also work in the Real case.

Theorem 6.1.

(Higson-Meyer-Thomsen) The functor kkKasG,sep:𝖦𝖢∗​𝖠𝗅𝗀sep→KKKasG,sep\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} is initial among functors to an additive 11-category which are reduced, homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable and split exact.

Remark 6.1.

The following remarks about Kasparov’s K​KGKK^{G}-theory are in order

  1. 1.

    It is a deep result of Kasparov ([40, Theorem 2.9]) that KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} has countable coproducts, and the functor kkKasG,sep\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}} takes countable direct sums in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to countable coproducts in KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}. An alternative proof using the Cuntz-Meyer picture of KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} can be given following [17, Corollary 11.16].

  2. 2.

    One can view the additive 11-category KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} as a half exact additive category by taking the maximal marking and taking the distinguished half exact sequences to be all short exact sequences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} admitting a equivariant cpc-split; the verification that this indeed is a half exact structure follows from [5, Section 7] (see also [28, Theorem 3.28] and the discussion above it).

  3. 3.

    KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} is a symmetric monoidal category and the functor kkKasG,sep:𝖦𝖢∗​𝖠𝗅𝗀sep→KKKasG,sep\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} has a symmetric monoidal refinement for both the minimal and the maximal tensor products on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}; this is explicitly stated in [23, Theorem 4.a]

Using Theorem 6.1, we can prove the comparison result between KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} and KKse,0G,sep\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{se},0}.

Theorem 6.2.

We have a natural equivalence of additive, symmetric monoidal (for both symmetric monoidal refinements) categories

KKse,0G,sep≃KKKasG,sep.\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{se},0}\simeq\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}.
Proof.

By construction, the canonical functor

kkse,0G,sep:𝖦𝖢∗​𝖠𝗅𝗀sep→KKse,0G,sep\mathrm{kk}^{G,\mathrm{sep}}_{\mathrm{se},0}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{se},0}

is reduced, homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, and additive. Thus, Theorem 6.1 says that there exists a unique additive functor ℱ:KKKasG,sep→KKse,0G,sep\mathcal{F}:\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}\rightarrow\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{se},0} such that ℱ∘kkKasG,sep=kkse,0G,sep\mathcal{F}\circ\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}=\mathrm{kk}^{G,\mathrm{sep}}_{\mathrm{se},0}.

On the other hand, the canonical functor

kkKasG,sep:𝖦𝖢∗​𝖠𝗅𝗀sep→KKKasG,sep\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}

is clearly reduced, homotopy invariant and 𝒦G{\mathcal{K}_{G}}-stable, as can be read off from Theorem 6.1. That it also satisfies the other hypothesis asked for in Section 3.4 is the content of Section 6.1. We thus obtain a unique functor 𝒢:KKse,0G,sep→KKKasG,sep\mathcal{G}:\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{se},0}\rightarrow\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} such that 𝒢∘kkse,0G,sep=KKKasG,sep\mathcal{G}\circ\mathrm{kk}^{G,\mathrm{sep}}_{\mathrm{se},0}=\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}. 𝒢\mathcal{G} is furthermore symmetric monoidal, as follows from the proof of Section 3.4 and [35, Proposition 3.3.2]. Our thesis now follows from a standard yoga with universal functors. ∎

Remark 6.2.

We implicitly used in the above proof the following basic facts: If 𝒞,𝒟\mathcal{C},\mathcal{D} are additive (resp. symmetric monoidal) categories, and F:𝒞→𝒟F:\mathcal{C}\rightarrow\mathcal{D} is an additive (resp. symmetric monoidal) functor which is an equivalence of the underlying categories, then the inverse is automatically additive (resp. symmetric monoidal).

We finally compare KKse,0G\mathrm{KK}^{G}_{\mathrm{se},0} with the classical non-separable extension of KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}, as described in [55, Definition 5.5] and [2, Section 2.1].

Proposition 6.2.

For A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and B∈𝖦𝖢∗​𝖠𝗅𝗀B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}, we have a natural isomorphism of abelian groups

KKKasG​(A,B)≅KKse,0G​(A,B).\mathrm{KK}^{G}_{\mathrm{Kas}}(A,B)\cong\mathrm{KK}^{G}_{\mathrm{se},0}(A,B).
Proof.

In light of Section 3.7, we have for AA and BB as in the statement of this proposition, an equivalence (with notation as in Section 3.7) of spectra

colimB′⊆sepBKKse,∞G(kkse,∞G(A),kkse,∞G(B′))→≃KKse,∞G(kkse,∞G(A),kkse,∞G(B))\displaystyle\operatorname{colim}_{B^{\prime}\subseteq_{\operatorname{sep}}B}\mathrm{KK}^{G}_{\mathrm{se},\infty}\bigl(\mathrm{kk}^{G}_{\mathrm{se},\infty}(A),\mathrm{kk}^{G}_{\mathrm{se},\infty}(B^{\prime})\bigr)\xrightarrow{\simeq}\mathrm{KK}^{G}_{\mathrm{se},\infty}\bigl(\mathrm{kk}^{G}_{\mathrm{se},\infty}(A),\mathrm{kk}^{G}_{\mathrm{se},\infty}(B)\bigr)

Since homotopy groups of spectra commute with filtered colimits, our thesis follows from the classical result that

colimB′⊆sepBKKKasG(A,B′)→≅KKKasG(A,B),\operatorname{colim}_{B^{\prime}\subseteq_{\operatorname{sep}}B}\mathrm{KK}^{G}_{\mathrm{Kas}}(A,B^{\prime})\xrightarrow{\cong}\mathrm{KK}^{G}_{\mathrm{Kas}}(A,B),

see for example [2, Lemma 2.1]. ∎

Remark 6.2.

When the C∗C^{*}-algebra AA in the first variable is not separable, KKse,0G​(A,−)\mathrm{KK}^{G}_{\mathrm{se},0}(A,-) need not coincide with KKKasG​(A,−)\mathrm{KK}^{G}_{\mathrm{Kas}}(A,-) a’la Skandalis; it boils down to the issue that homotopy groups of homotopy limits need not be limits of homotopy groups.

6.2 Recapitulation of classical ungraded EGE^{G}-theory (with some details)

Just as in the last subsection, we begin by recalling the classical definitions of the ungraded (Real) EGE^{G}-categories.

Classically, ungraded EGE^{G}-theory was defined in terms of asymptotic morphisms by Connes-Higson in [20]. The foundational works on (equivariant) EE-theory ([20], [29], [34]) did not discuss the Real structure, and the author (of this article) is only aware of Boersema’s work [9] on the same 4040 40 which was pointed out to him by Yuezhao Li. However, loc.​ cit.​ does not discuss equivariant matters. Note that although [9] is written with real C∗C^{*}-algebras, the modifications to the Real case are obvious.

In the remainder of this subsection, we will therefore be making a comparison of KKex,0G,sep\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{ex},0} with a equivariant version of Boersema’s (Real) EE-category. The complex situation can be dealt similarly, and with lesser difficulties. Note that we omit a discussion of non-separable EE-theory (the analogues of Section 6.1 and Section 6.1 hold in this context too). Therefore, we use the notation EclassG\mathrm{E}^{G}_{\mathrm{class}} to always denote the separable theory.

We begin with the key definitions.

Definition 6.2.
  1. 1.

    Let A,B∈𝖦𝖢∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. An asymptotic morphism from AA to BB is a one-parameter family of functions φt:A→B\varphi_{t}:A\to B with t∈[1,∞)t\in[1,\infty), satisfying the continuity condition that for all a∈Aa\in A, the map

    t⟼φt​(a):[1,∞)→Bt\longmapsto\varphi_{t}(a):[1,\infty)\to B

    is bounded and continuous, and the asymptotic conditions that for all a,a1,a2∈Aa,a_{1},a_{2}\in A and λ∈ℂ\lambda\in\mathbb{C}

    φt​(a1​a2)−φt​(a1)​φt​(a2)φt​(a1+a2)−φt​(a1)−φt​(a2)φt​(λ​a)−λ​φt​(a)φt​(a∗)−φt​(a)∗φt(g.a)−g.φt(a)}→0,as ​t→∞\begin{cases}\varphi_{t}(a_{1}a_{2})-\varphi_{t}(a_{1})\varphi_{t}(a_{2})\\ \varphi_{t}(a_{1}+a_{2})-\varphi_{t}(a_{1})-\varphi_{t}(a_{2})\\ \varphi_{t}(\lambda a)-\lambda\varphi_{t}(a)\\ \varphi_{t}(a^{*})-\varphi_{t}(a)^{*}\\ \varphi_{t}(g.a)-g.\varphi_{t}(a)\end{cases}\to 0,\qquad\text{as }t\to\infty

    When AA and BB are Real, we shall require that in addition

    τ⁡(φt​(a))−φt​(τ⁡(a))→0as ​t→∞.\tau(\varphi_{t}(a))-\varphi_{t}(\tau(a))\to 0\qquad\text{as }t\to\infty.

    We shall denote an asymptotic morphism φ:A⇢B\varphi:A\dashrightarrow B with a dashed arrow.

  2. 2.

    There is a natural notion of homotopy between asymptotic morphisms which is an equivalence relation (see [29, Chapter 2]), and we denote by [[A,B]]G[[A,B]]_{G} the GG-equivariant asymptotic homotopy classes of maps4141 41 as in the ordinary homotopy case, if the external group GG is clear from the context, we omit it from the notation. from AA to BB. This forms a category AsyG\Asy^{G}, whose objects are separable GG-C∗C^{*}-algebras, and morphisms are GG-equivariant asymptotic homotopy classes of maps.

  3. 3.

    Just as the passage from 𝖦𝖢∗​𝖠𝗅𝗀hsep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} to S𝒦G​𝖦𝖢∗​𝖠𝗅𝗀hsep\mathrm{S}_{{\mathcal{K}_{G}}}\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}_{h}^{\mathrm{sep}} (see Section 3.2.1), one can form the category S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G} via left and right Bousfield localizations of AsyG\Asy^{G}, whose hom monoids would be 𝒦G{\mathcal{K}_{G}}-stabilized asymptotic homotopy classes of maps.

    Note that AsyG\Asy^{G} and S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G} are 11-categories; an ∞\infty-categorical refinement of these categories has been studied in [11] when GG is a discrete countable group. The methods of loc.​ cit.​ would not generalize to general locally compact second countable groups. We anyway work only with the 11-categorical variants in this section.

  4. 4.

    The classical EGE^{G}-groups are given by

    EclassG​(A,B):=homS𝒦G​AsyG⁡(Ω​A,Ω​B)=[[Ω​A⊗𝒦G,Ω​B⊗𝒦G]],\mathrm{E}^{G}_{\mathrm{class}}(A,B):=\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(\Omega A,\Omega B)=[[\Omega A\otimes{\mathcal{K}_{G}},\Omega B\otimes{\mathcal{K}_{G}}]],

    and yield a symmetric monoidal additive category structure on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} with respect to the maximal tensor product on 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. That it indeed becomes a symmetric monoidal additive category can be seen by combining the approaches and relevant results of [29] and [9]. There is an obvious functor

    eclassG:𝖦𝖢∗​𝖠𝗅𝗀sep→EclassG.\mathrm{e}^{G}_{\mathrm{class}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{E}^{G}_{\mathrm{class}}.
  5. 5.

    One can view the additive 11-category EclassG\mathrm{E}^{G}_{\mathrm{class}} as a half exact additive category by taking the maximal marking and taking the distinguished half exact sequences to be all short exact sequences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}; see Section 6.2.3 for details. In the remainder of this subsection, we by default work with this half exact structure.

For later use, we mention a few technical results about asymptotic morphisms now. In the non-equivariant case, some of these results are also discussed in the PhD thesis of Andreas Thom ([57, Section 2.2]) with a little more elaborations.

Lemma 6.2.

Let A,B∈𝖦𝖢∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. Denote by [[A,B]]~\widetilde{[[A,B]]} the set of homotopy classes of asymptotic morphisms φ:A⇢B\varphi:A\dashrightarrow B which have the property that φ1​(a)=0​∀a∈A\varphi_{1}(a)=0\penalty\ \forall\penalty\ a\in A. Homotopies are also required to satisfy this condition. Then the natural map

ΦA,B:[[A,B]]~→[[A,B]]\Phi_{A,B}:\widetilde{[[A,B]]}\rightarrow[[A,B]]

is an isomorphism.

Proof.

We just write a map in the other direction; that it is well-defined and inverse to ΦA,B\Phi_{A,B} is a routine check.

Fix a function f:[1,∞)→[0,1]f:[1,\infty)\rightarrow[0,1] with the property that f⁡(1)=0,f⁡(t)=1​∀t≥2f(1)=0,f(t)=1\penalty\ \forall\penalty\ t\geq 2. Then the pointwise multiplication of ff with an element of [[A,B]][[A,B]] does the job. ∎

The above lemma has the following interesting consequence. For B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, denote by C0​b​([1,∞),B)C_{0b}([1,\infty),B) the (non-separable) GG-C∗C^{*}-algebra of GG-continuous, continuous, bounded functions f:[1,∞)→Bf:[1,\infty)\rightarrow B which further satisfy f⁡(1)=0f(1)=0. Section 6.2 shows that the datum of an (equivalence class) of an asymptotic morphism A⇢BA\dashrightarrow B is the same datum as a GG-equivariant homomorphism A→C0​b​([1,∞),B)C0​((1,∞),B)A\rightarrow\frac{C_{0b}([1,\infty),B)}{C_{0}((1,\infty),B)}. Thus, we can naturally associate to an asymptotic morphism φ:A⇢B\varphi:A\dashrightarrow B the extension given in the top row of the diagram

0{\lx@inpgf@ignorespaces 0}C0​((1,∞),B){\lx@inpgf@ignorespaces{C_{0}((1,\infty),B)}}Pφ{\lx@inpgf@ignorespaces{P_{\varphi}}}A{\lx@inpgf@ignorespaces A}0{\lx@inpgf@ignorespaces 0}0{\lx@inpgf@ignorespaces 0}C0​((1,∞),B){\lx@inpgf@ignorespaces{C_{0}((1,\infty),B)}}C0​b​([1,∞),B){\lx@inpgf@ignorespaces{C_{0b}([1,\infty),B)}}C0​b​([1,∞),B)C0​((1,∞),B){\lx@inpgf@ignorespaces{\frac{C_{0b}([1,\infty),B)}{C_{0}((1,\infty),B)}}}0{\lx@inpgf@ignorespaces 0}=\scriptstyle{\lx@inpgf@ignorespaces=}φ\scriptstyle{\lx@inpgf@ignorespaces\varphi} (6.3)

where the right square is a pullback. Note that Pφ∈𝖦𝖢∗​𝖠𝗅𝗀sepP_{\varphi}\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} courtesy both C0​((1,∞),B)C_{0}((1,\infty),B) and AA being separable.

Lemma 6.3.

In the notation of the above discussion, let ψ:Ω​A⇢Ω​B\psi:\Omega A\dashrightarrow\Omega B be the asymptotic morphism obtained by applying the equivariant (Real) Connes-Higson construction ([29, Proposition 5.5], [9, Proposition 4.3]) to the top extension in Equation 6.3. Then [ψ]=−[Ω​φ][\psi]=-[\Omega\varphi] in [[Ω​A,Ω​B]][[\Omega A,\Omega B]].

Proof.

This is the content of [37, Lemma 1.3], see also [59, Lemma 3.4]. Note that there is a sign error in the analogous assertion [29, Proposition 5.12]. ∎

Our first important result of this subsection is to prove the following theorem, which is folklore even in the complex case: to the best of the author’s knowledge, the classical literature on EE-theory just state the result without a proof; see also [11, Remark 3.33].

Theorem 6.4.

(folklore) The functor eclassG:𝖦𝖢∗​𝖠𝗅𝗀sep→EclassG\mathrm{e}^{G}_{\mathrm{class}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{E}^{G}_{\mathrm{class}} is initial among functors to an additive 11-category which are reduced, homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable and half exact.

A (detailed) proof of the above result will take us quite some time. We begin with some preparations. The first check one needs to make to prove Theorem 6.4 is that eclassG:𝖦𝖢∗​𝖠𝗅𝗀sep→EclassG\mathrm{e}^{G}_{\mathrm{class}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{E}^{G}_{\mathrm{class}} is homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable and exact. While the first two are obvious from the definition, half exactness is not so. The first crucial step to that end is demonstrating for each A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the functor

EclassG​(A,−):𝖦𝖢∗​𝖠𝗅𝗀sep→Ab\mathrm{E}^{G}_{\mathrm{class}}(A,-):\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\operatorname{Ab}

is split exact. This follows directly from the equivariant, Real analogue of [8, Corollary 25.5.7]. However, it can also be seen as a consequence of the following stronger result, which is also going to come handy in the next subsection. The complex, non-equivariant case of the result is due to Dadarlat-Loring ([24, Proposition 3.2]).

Proposition 6.4.

For each D∈𝖦𝖢∗​𝖠𝗅𝗀sepD\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the functor [[D,−]]:𝖦𝖢∗​𝖠𝗅𝗀sep→Set∗[[D,-]]:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\operatorname{Set}_{*} is split exact.

Proof.

Let 0→A→B→𝑓C→00\rightarrow A\rightarrow B\xrightarrow{f}C\rightarrow 0 be a short exact sequence in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} which is split by a homomorphism σ:C→B\sigma:C\rightarrow B. Without loss of generality, we can assume that the map A→BA\rightarrow B is the inclusion of an ideal. From the standard excision properties in the asymptotic category and Puppe sequences in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}},([29, Proposition 5.16], [32, Proposition 2.5]), we get a long exact sequence of pointed sets

...→[[D,ΩB]]→Ω​f∗[[D,ΩC]]→∂[[D,C(f)]]→[[D,B]]→f∗[[D,C]]→0...\rightarrow[[D,\Omega B]]\xrightarrow{\Omega f_{*}}[[D,\Omega C]]\xrightarrow{\partial}[[D,C(f)]]\rightarrow[[D,B]]\xrightarrow{f_{*}}[[D,C]]\rightarrow 0 (6.5)

where C⁡(f)C(f) denotes the mapping cone of ff. Since ff is split by σ\sigma, Ω​f\Omega f is split by Ω​σ\Omega\sigma, and we can extract the split exact sequence

0→[[D,C⁡(f)]]→[[D,B]]→f∗[[D,C]]→00\rightarrow[[D,C(f)]]\rightarrow[[D,B]]\xrightarrow{f_{*}}[[D,C]]\rightarrow 0

from Equation 6.5. To prove our thesis, it therefore suffices to show that the inclusion A→C⁡(f)A\rightarrow C(f) is an isomorphism in AsyG\Asy^{G}.

Using the split σ\sigma, we can re-write C⁡(f)C(f) as

C⁡(f)={(a+σ⁡(γ⁡(0)),γ)∣a∈A}⊆B⊕P​C.C(f)=\{(a+\sigma(\gamma(0)),\gamma)\mid a\in A\}\subseteq B\oplus PC.

Let utu_{t} be a (Real) quasicentral approximate unit in AA ([29, Lemma 5.3]). In light of [29, Lemma 5.6.(iii)], we can now define a 11-parameter family of homomorphisms

φt:C0(0,1]\displaystyle\varphi_{t}:C_{0}(0,1] →A\displaystyle\rightarrow A
f\displaystyle f ↦f⁡(ut)\displaystyle\mapsto f(u_{t})

given by functional calculi of the individual utu_{t}. We can now define an asymptotic morphism given by the family of maps

ρt:C0(0,1]⊗C\displaystyle\rho_{t}:C_{0}(0,1]\otimes C →A\displaystyle\rightarrow A
f⊗c\displaystyle f\otimes c ↦f⁡(ut)​σ​(c)\displaystyle\mapsto f(u_{t})\sigma(c)

Note that in defining it, we used the universal property of the maximal tensor product, see [8, Section 25.2.3]. We can now define an asymptotic morphism φ:C⁡(f)⇢A\varphi:C(f)\dashrightarrow A given by

φt​(a+σ⁡(γ⁡(0)),γ)=a+ρt​(f).\varphi_{t}(a+\sigma(\gamma(0)),\gamma)=a+\rho_{t}(f).

The verification that it indeed is an inverse to the inclusion A→C⁡(f)A\rightarrow C(f) in AsyG\Asy^{G} can now be taken from the proof of [24, Proposition 3.2]. The equivariance and Real structure do not pose any additional difficulties. ∎

As the reader may guess, the reason we care about the split exactness result is to bring KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} (or equivalently, KK!,0G,sep\mathrm{KK}_{!,0}^{G,\mathrm{sep}}) into the game. From results of the previous subsection and playing around a bit with the uniqueness of universal functors ([9, Theorem 3.2]), we conclude that there is a unique functor c:KK!,0G,sep→EGclassc:\mathrm{KK}_{!,0}^{G,\mathrm{sep}}\rightarrow\mathrm{E}^{G}_{\mathrm{class}} such that c∘kk!,0G,sep=eGclassc\circ\mathrm{kk}_{!,0}^{G,\mathrm{sep}}=\mathrm{e}^{G}_{\mathrm{class}} 4242 42 c stands for comparison functor, which is furthermore symmetric monoidal with respect to the maximal tensor product.

Since we already have knowledge of periodicity in KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}} (equivalently, in KK!,0G,sep\mathrm{KK}_{!,0}^{G,\mathrm{sep}}), we can now get periodicity results in EclassG\mathrm{E}^{G}_{\mathrm{class}} too. All this (and a little more) is the content of the next lemma.

Lemma 6.5.
  1. 1.

    Let F:𝖦𝖢∗​𝖠𝗅𝗀sep→𝒟F:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathcal{D} be a functor to a half exact additive 11-category which is homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, half exact with respect to exact sequences. Then there is an isomorphism

    F⁡(C0​(ℝ2,2)⊗A)→≅BottFF⁡(A)F(C_{0}(\mathbb{R}^{2,2})\otimes A)\xrightarrow[\cong]{\operatorname{Bott}^{F}}F(A)

    which is natural with respect to morphisms in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and also with respect to the boundary maps of the long exact sequence associated to FF, as described in [8, Theorem 21.4.4].

  2. 2.

    The natural map

    C0(ℝ0,1)⊗−:EclassG(A,B)→EclassG(ΩA,ΩB)C_{0}(\mathbb{R}^{0,1})\otimes-:\mathrm{E}^{G}_{\mathrm{class}}(A,B)\rightarrow\mathrm{E}^{G}_{\mathrm{class}}(\Omega A,\Omega B)

    is an isomorphism.

  3. 3.

    The functor eclassG:𝖦𝖢∗​𝖠𝗅𝗀sep→EclassG\mathrm{e}^{G}_{\mathrm{class}}:\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\mathrm{E}^{G}_{\mathrm{class}} is homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable, and half exact.

  4. 4.

    The natural map

    C0(ℝ1,0)⊗−:EclassG(A,B)→EclassG(C0(ℝ1,0)⊗A,C0(ℝ1,0)⊗B)C_{0}(\mathbb{R}^{1,0})\otimes-:\mathrm{E}^{G}_{\mathrm{class}}(A,B)\rightarrow\mathrm{E}^{G}_{\mathrm{class}}(C_{0}(\mathbb{R}^{1,0})\otimes A,C_{0}(\mathbb{R}^{1,0})\otimes B)

    is an isomorphism.

  5. 5.

    The isomorphisms of Assertion 1 applied to the functors EclassG​(A,−)\mathrm{E}^{G}_{\mathrm{class}}(A,-) and EclassG​(−,C0​(ℝ2,2)⊗B)\mathrm{E}^{G}_{\mathrm{class}}(-,C_{0}(\mathbb{R}^{2,2})\otimes B) fit into a commutative diagram

    EclassG​(C0​(ℝ2,2)⊗A,C0​(ℝ2,2)⊗B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(C_{0}(\mathbb{R}^{2,2})\otimes A,C_{0}(\mathbb{R}^{2,2})\otimes B)}}EclassG​(A,B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,B)}}EclassG​(A,C0​(ℝ2,2)⊗B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,C_{0}(\mathbb{R}^{2,2})\otimes B)}}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}C0(ℝ2,2)⊗−\scriptstyle{\lx@inpgf@ignorespaces C_{0}(\mathbb{R}^{2,2})\otimes-}≅\scriptstyle{\lx@inpgf@ignorespaces\cong}
Proof.

We begin with Assertion 1. In light of the given properties of FF, the Real analog of the proof of [29, Proposition 6.16] shows that there exists an asymptotic morphism

α:C0​(ℝ1,1)⇢𝒦⁡(l2​ℕ)\alpha:C_{0}(\mathbb{R}^{1,1})\dashrightarrow\mathcal{K}(l^{2}\mathbb{N})

such that for each A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, the asymptotic morphism

α⊗1A:C0​(ℝ1,1)⊗A⇢𝒦⁡(l2​ℕ)⊗A\alpha\otimes 1_{A}:C_{0}(\mathbb{R}^{1,1})\otimes A\dashrightarrow\mathcal{K}(l^{2}\mathbb{N})\otimes A

yields a natural isomorphism

F⁡(C0​(ℝ1,1)⊗A)→≅BottAFF⁡(A).F(C_{0}(\mathbb{R}^{1,1})\otimes A)\xrightarrow[\cong]{\operatorname{Bott}_{A}^{F}}F(A).

Our sought after natural map is now obtained by applying the above isomorphism twice

F⁡(C0​(ℝ2,2)⊗A)→≅BottC0​(ℝ1,1)⊗AFF⁡(C0​(ℝ1,1)⊗A)→≅BottAFF⁡(A).F(C_{0}(\mathbb{R}^{2,2})\otimes A)\xrightarrow[\cong]{\operatorname{Bott}_{C_{0}(\mathbb{R}^{1,1})\otimes A}^{F}}F(C_{0}(\mathbb{R}^{1,1})\otimes A)\xrightarrow[\cong]{\operatorname{Bott}_{A}^{F}}F(A).

The map in Assertion 2 being an isomorphism can be readily taken from [9, Lemma 4.5], with the obvious modifications to tackle the equivariant case.

We now prove Assertion 3 (note that it settles the easy part of Theorem 6.4). That eclassG\mathrm{e}^{G}_{\mathrm{class}} is homotopy invariant and 𝒦G{\mathcal{K}_{G}}-stable is obvious. That it is also half exact follows by combining [9, Theorem 4.4] and the excision theory of equivariant EE-theory developed in chapters 5 and 6 of [29]. The careful reader will observe that (variants of) Assertions 1 and 2 go as an input to proving the exactness in the first variable in [9] and [29].

For Assertion 4, we can accommodate the map in the commutative diagram

EclassG​(A,B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,B)}}EclassG​(C0​(ℝ1,1)⊗A,C0​(ℝ1,1)⊗B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(C_{0}(\mathbb{R}^{1,1})\otimes A,C_{0}(\mathbb{R}^{1,1})\otimes B)}}EclassG​(C0​(ℝ1,0)⊗A,C0​(ℝ1,0)⊗B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(C_{0}(\mathbb{R}^{1,0})\otimes A,C_{0}(\mathbb{R}^{1,0})\otimes B)}}C0(ℝ1,1)⊗−\scriptstyle{\lx@inpgf@ignorespaces C_{0}(\mathbb{R}^{1,1})\otimes-}C0(ℝ1,0)⊗−\scriptstyle{\lx@inpgf@ignorespaces C_{0}(\mathbb{R}^{1,0})\otimes-}C0(ℝ0,1)⊗−\scriptstyle{\lx@inpgf@ignorespaces C_{0}(\mathbb{R}^{0,1})\otimes-}

The discussion preceding the lemma shows that the horizontal arrow is an isomorphism, since

C0(ℝ1,1)≃KKKasG,sepℂ.C_{0}(\mathbb{R}^{1,1})\simeq_{\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}}\mathbb{C}.

The right arrow is an isomorphism from Assertion 2.

Finally we show Assertion 5. In light of Assertion 1, it essentially follows from the commutativity of the diagram

C0​(ℝ1,1)⊗A{\lx@inpgf@ignorespaces{C_{0}(\mathbb{R}^{1,1})\otimes A}}𝒦⁡(l2​ℕ)⊗A{\lx@inpgf@ignorespaces{\mathcal{K}(l^{2}\mathbb{N})\otimes A}}C0​(ℝ1,1)⊗B{\lx@inpgf@ignorespaces{C_{0}(\mathbb{R}^{1,1})\otimes B}}𝒦⁡(l2​ℕ)⊗B{\lx@inpgf@ignorespaces{\mathcal{K}(l^{2}\mathbb{N})\otimes B}}α⊗1A\scriptstyle{\lx@inpgf@ignorespaces\alpha\otimes 1_{A}}1C0​(ℝ1,1)⊗f\scriptstyle{\lx@inpgf@ignorespaces 1_{C_{0}(\mathbb{R}^{1,1})}\otimes f}1𝒦⁡(l2​ℕ)⊗f\scriptstyle{\lx@inpgf@ignorespaces 1_{\mathcal{K}(l^{2}\mathbb{N})}\otimes f}α⊗1B\scriptstyle{\lx@inpgf@ignorespaces\alpha\otimes 1_{B}}

for every asympototic morphism f:A⇢Bf:A\dashrightarrow B, as can be seen from the symmetric monoidal properties of AsyG\Asy^{G}. See also [29, Theorem 4.6] and the proof of [29, Proposition 6.16]. ∎

Before continuing with the proof of Theorem 6.4, we mention a corollary to some results of the last lemma, which will come handy in the next section.

Corollary 6.5.

There exists an asymptotic morphism α:C0​(ℝ1,1)⇢𝒦⁡(l2)\alpha:C_{0}(\mathbb{R}^{1,1})\dashrightarrow\mathcal{K}(l^{2}) such that

α⊗1B:C0​(ℝ1,1)⊗B⇢𝒦⁡(l2)⊗B\alpha\otimes 1_{B}:C_{0}(\mathbb{R}^{1,1})\otimes B\dashrightarrow\mathcal{K}(l^{2})\otimes B

determines an invertible class in EclassG​(C0​(ℝ1,1)⊗B,B)\mathrm{E}^{G}_{\mathrm{class}}(C_{0}(\mathbb{R}^{1,1})\otimes B,B). Furthermore, the functor

Ω:S𝒦G​AsyG→EclassG\Omega:\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}\rightarrow\mathrm{E}^{G}_{\mathrm{class}}

exhibits EclassG\mathrm{E}^{G}_{\mathrm{class}} as the 11-categorical localization of S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G} at the classes of maps α⊗1B\alpha\otimes 1_{B}.

Proof.

The first statement follows readily from the proof of Assertion 1 of Section 6.2 by taking 𝒟=EclassG\mathcal{D}=\mathrm{E}^{G}_{\mathrm{class}}. The second statement follows from the following general fact about (∞−)(\infty-)categories (it is the dual version of [43, Proposition 5.2.7.4]) : Let 𝒞\mathcal{C} be a category with an endofunctor R:𝒞→𝒞R:\mathcal{C}\rightarrow\mathcal{C} and a natural transformation 𝔗:R⟹id𝒞\mathfrak{T}:R\implies\operatorname{id}_{\mathcal{C}}. If for every object C∈𝒞C\in\mathcal{C} the morphims

𝔗R⁡(C),R⁡(𝔗C):R⁡(R⁡(C))→R⁡(C)\mathfrak{T}_{R(C)},R(\mathfrak{T}_{C}):R(R(C))\rightarrow R(C)

are equivalences, then R:𝒞→R​𝒞R:\mathcal{C}\rightarrow R\mathcal{C} is the right-adjoint of a right Bousfield localization with counit 𝔗\mathfrak{T}. It is also the Dwyer-Kan localization at the set of morphisms WR:={𝔗C∣C∈𝒞}W_{R}:=\{\mathfrak{T}_{C}\mid C\in\mathcal{C}\}.

Indeed, in the above notation, take 𝒞:=S𝒦G​AsyG\mathcal{C}:=\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}, and R:=C0(ℝ1,1)⊗−:S𝒦GAsyG→S𝒦GAsyGR:=C_{0}(\mathbb{R}^{1,1})\otimes-:\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}\rightarrow\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}. The rest follows from the results of Section 6.2 and the definition of EclassG\mathrm{E}^{G}_{\mathrm{class}}. ∎

The heart of the proof of the uniqueness assertion in Theorem 6.4 is contained in the following result.

Proposition 6.5.

(cf. [59, Theorem 4.6]) Let FF be a homotopy invariant, 𝒦G{\mathcal{K}_{G}}-stable and half exact functor from 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to Ab\operatorname{Ab}. Fix AA in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and consider an arbitrary element d∈F⁡(A)d\in F(A). Then there is a unique natural transformation

T:EclassG​(A,−)⟹F⁡(−)T:\mathrm{E}^{G}_{\mathrm{class}}(A,-)\implies F(-)

such that TA​([idA])=dT_{A}([\operatorname{id}_{A}])=d.

Proof.

Firstly, we massage the hom groups of EclassG\mathrm{E}^{G}_{\mathrm{class}} a bit, and write them as

EclassG​(A,B)=[[C0​(ℝ2,1)⊗A⊗𝒦G,C0​(ℝ2,1)⊗B⊗𝒦G]].\mathrm{E}^{G}_{\mathrm{class}}(A,B)=[[C_{0}(\mathbb{R}^{2,1})\otimes A\otimes{\mathcal{K}_{G}},C_{0}(\mathbb{R}^{2,1})\otimes B\otimes{\mathcal{K}_{G}}]].

Indeed this can be done from Assertions 2 and 4 of Section 6.2 (the reason we do this maneuver will be clear from the upcoming proof, but see also Section 6.2).

To avoid notational clutter, we subsequently denote C0​(ℝp,q)⊗XC_{0}(\mathbb{R}^{p,q})\otimes X as ℝp,q​X\mathbb{R}^{p,q}X for any X∈𝖦𝖢∗​𝖠𝗅𝗀sepX\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. Same comment applies to functors involving these algebras.

Now consider x∈[[ℝ2,1​A⊗𝒦G,ℝ2,1​B⊗𝒦G]]x\in[[\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}B\otimes{\mathcal{K}_{G}}]]. Let it be represented by the equivariant asymptotic morphism

φ:ℝ2,1​A⊗𝒦G⇢ℝ2,1​B⊗𝒦G.\varphi:\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}}\dashrightarrow\mathbb{R}^{2,1}B\otimes{\mathcal{K}_{G}}.

As in Equation 6.3, this yields an extension

0→ℝ2,2​B⊗𝒦G→Pφ→ℝ2,1​A⊗𝒦G→0.0\rightarrow\mathbb{R}^{2,2}B\otimes{\mathcal{K}_{G}}\rightarrow P_{\varphi}\rightarrow\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}}\rightarrow 0. (6.6)

Consequently, we obtain a morphism F⁡(ℝ2,2​A⊗𝒦G)→F⁡(ℝ2,2​B⊗𝒦G)F(\mathbb{R}^{2,2}A\otimes{\mathcal{K}_{G}})\rightarrow F(\mathbb{R}^{2,2}B\otimes{\mathcal{K}_{G}}) in Ab\operatorname{Ab} via the connecting map of the long exact sequence associated to FF as in [8, Theorem 21.4.4]. The 𝒦G{\mathcal{K}_{G}}-stability of FF together with Assertion 1 of Section 6.2 naturally produces a morphism Tx:F⁡(A)→F⁡(B)T_{x}:F(A)\rightarrow F(B). Now define

TB:[[ℝ2,1​A⊗𝒦G,ℝ2,1​B⊗𝒦G]]→F⁡(B)\displaystyle T_{B}:[[\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}B\otimes{\mathcal{K}_{G}}]]\rightarrow F(B)
x↦Tx​(d).\displaystyle x\mapsto T_{x}(d).

In light of the machinery we developed in this subsection and functoriality properties of the Connes-Higson construction, the well-definedness and naturality of TBT_{B}, as well as the verification TA​([idA])=dT_{A}([\operatorname{id}_{A}])=d is a routine check, as has been done in the proof of [59, Theorem 4.6].

We now prove the uniqueness part. Let

T′:[[ℝ2,1A⊗𝒦G,ℝ2,1−⊗𝒦G]]→F(−)T^{\prime}:[[\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}-\otimes{\mathcal{K}_{G}}]]\rightarrow F(-)

be a natural transformation such that T′​([idA])=dT^{\prime}([\operatorname{id}_{A}])=d. Consider x=[φ]∈[[ℝ2,1​A⊗𝒦G,ℝ2,1​B⊗𝒦G]]x=[\varphi]\in[[\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}B\otimes{\mathcal{K}_{G}}]]. Let ∂1,∂2,∂3,∂4\partial_{1},\partial_{2},\partial_{3},\partial_{4} denote the connecting maps obtained by applying the functors

[[ℝ4,3​A⊗𝒦G,ℝ2,1−]],[[ℝ2,1​A⊗𝒦G,ℝ2,1−]],F⁡(ℝ2,2−),F⁡(−)[[\mathbb{R}^{4,3}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}-]],[[\mathbb{R}^{2,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{2,1}-]],F(\mathbb{R}^{2,2}-),F(-)

respectively to the extension in Equation 6.64343 43 denoting by 𝒢\mathcal{G} any one of these four functors, we are implicitly using the natural identification of 𝒢⁡(−)\mathcal{G}(-) with 𝒢(ℝ2,2⊗𝒦G⊗−)\mathcal{G}(\mathbb{R}^{2,2}\otimes{\mathcal{K}_{G}}\otimes-) in what follows.. We get a commutative diagram

EclassG​(ℝ2,2​A,ℝ2,2​A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}A)}}EclassG​(ℝ2,2​A,ℝ2,2​B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}B)}}EclassG​(A,A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,A)}}EclassG​(A,ℝ2,2​A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,\mathbb{R}^{2,2}A)}}EclassG​(A,ℝ2,2​B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,\mathbb{R}^{2,2}B)}}EclassG​(A,B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,B)}}F⁡(ℝ2,2​A){\lx@inpgf@ignorespaces{F(\mathbb{R}^{2,2}A)}}F⁡(ℝ2,2​B){\lx@inpgf@ignorespaces{F(\mathbb{R}^{2,2}B)}}F⁡(A){\lx@inpgf@ignorespaces{F(A)}}F⁡(B){\lx@inpgf@ignorespaces{F(B)}}∂1\scriptstyle{\color[rgb]{0.3608,0.3608,0.8392}\lx@inpgf@ignorespaces\partial_{1}}BottEclassG​(−,ℝ2,2​A)\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{E^{G}_{\operatorname{class}}(-,\mathbb{R}^{2,2}A)}}BottEclassG​(−,ℝ2,2​B)\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{E^{G}_{\operatorname{class}}(-,\mathbb{R}^{2,2}B)}}ℝ2,2−\scriptstyle{\color[rgb]{0.3608,0.3608,0.8392}\lx@inpgf@ignorespaces\mathbb{R}^{2,2}-}BottEclassG​(A,−)\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{E^{G}_{\operatorname{class}}(A,-)}}TA′\scriptstyle{\lx@inpgf@ignorespaces T^{\prime}_{A}}∂2\scriptstyle{\lx@inpgf@ignorespaces\partial_{2}}Tℝ2,2​A′\scriptstyle{\lx@inpgf@ignorespaces T^{\prime}_{\mathbb{R}^{2,2}A}}BottEclassG​(A,−)\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{E^{G}_{\operatorname{class}}(A,-)}}Tℝ2,2​B′\scriptstyle{\lx@inpgf@ignorespaces T^{\prime}_{\mathbb{R}^{2,2}B}}ℝ2,2−\scriptstyle{\color[rgb]{0.3608,0.3608,0.8392}\lx@inpgf@ignorespaces\mathbb{R}^{2,2}-}TB′\scriptstyle{\lx@inpgf@ignorespaces T^{\prime}_{B}}∂3\scriptstyle{\lx@inpgf@ignorespaces\partial_{3}}BottF\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{F}}BottF\scriptstyle{\lx@inpgf@ignorespaces\operatorname{Bott}^{F}}∂4\scriptstyle{\lx@inpgf@ignorespaces\partial_{4}} (6.7)

where the undirected edges are induced by the maps described in Section 6.2.1. Note that the fact that the diagram indeed commutes needs a lot of the machinery we developed earlier in this subsection.

We now claim the following.

Claim.

The composite

∂1∘(ℝ2,2−):EclassG(A,A)→EclassG(ℝ2,2A,ℝ2,2B)\partial_{1}\circ(\mathbb{R}^{2,2}-):\mathrm{E}^{G}_{\mathrm{class}}(A,A)\rightarrow\mathrm{E}^{G}_{\mathrm{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}B)

equals the composite

(ℝ2,2−)∘φ∗:EclassG​(A,A)→EclassG​(ℝ2,2​A,ℝ2,2​B).(\mathbb{R}^{2,2}-)\circ\varphi_{*}:\mathrm{E}^{G}_{\mathrm{class}}(A,A)\rightarrow\mathrm{E}^{G}_{\mathrm{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}B).
Proof.

We build the diagram

EclassG​(ℝ2,2​A,ℝ2,2​A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}A)}}EclassG​(ℝ2,2​A,ℝ2,2​B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,2}A,\mathbb{R}^{2,2}B)}}EclassG​(ℝ2,1​A,ℝ2,1​A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,1}A,\mathbb{R}^{2,1}A)}}EclassG​(ℝ2,1​A,ℝ2,1​B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,1}A,\mathbb{R}^{2,1}B)}}EclassG​(ℝ2,0​A,ℝ2,0​A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,0}A,\mathbb{R}^{2,0}A)}}EclassG​(ℝ2,0​A,ℝ2,0​B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\mathbb{R}^{2,0}A,\mathbb{R}^{2,0}B)}}EclassG​(A,A){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,A)}}EclassG​(A,B){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A,B)}}∂1\scriptstyle{\lx@inpgf@ignorespaces\partial_{1}}ℝ0,1−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{0,1}-}−∂[[ℝ4,2A⊗𝒦G,ℝ2,0−⊗𝒦G]]\scriptstyle{\lx@inpgf@ignorespaces-\partial_{[[\mathbb{R}^{4,2}A\otimes\mathcal{K}_{G},\mathbb{R}^{2,0}-\otimes\mathcal{K}_{G}]]}}ℝ0,1−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{0,1}-}ℝ0,1−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{0,1}-}(ℝ2,0​φ)∗\scriptstyle{\lx@inpgf@ignorespaces(\mathbb{R}^{2,0}\varphi)_{*}}ℝ0,1−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{0,1}-}ℝ2,0−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{2,0}-}φ∗\scriptstyle{\lx@inpgf@ignorespaces\varphi_{*}}ℝ2,0−\scriptstyle{\lx@inpgf@ignorespaces\mathbb{R}^{2,0}-}

We need to show that it commutes. The bottom rectangle commutes by the symmetric monoidal properties of EclassG\mathrm{E}^{G}_{\mathrm{class}}. The middle rectangle commutes by an application of Section 6.2, together with the fact that composition with the Connes-Higson morphism yields the boundary map in EclassG\mathrm{E}^{G}_{\mathrm{class}}, as described in [29, Theorem 6.15]. The top square commuting is a consequence of the general fact that for any A′,B′,C′∈𝖦𝖢∗​𝖠𝗅𝗀sepA^{\prime},B^{\prime},C^{\prime}\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} and ψ∈EclassG​(B′,C′)\psi\in\mathrm{E}^{G}_{\mathrm{class}}(B^{\prime},C^{\prime}), the diagram

EclassG​(Ω​A′,Ω​B′){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\Omega A^{\prime},\Omega B^{\prime})}}EclassG​(Ω​B′,Ω​C′){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(\Omega B^{\prime},\Omega C^{\prime})}}EclassG​(A′,B′){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(A^{\prime},B^{\prime})}}EclassG​(B′,C′){\lx@inpgf@ignorespaces{E^{G}_{\operatorname{class}}(B^{\prime},C^{\prime})}}−Ω​ψ∗\scriptstyle{\lx@inpgf@ignorespaces-\Omega\psi_{*}}Ω∗\scriptstyle{\lx@inpgf@ignorespaces\Omega_{*}}ψ∗\scriptstyle{\lx@inpgf@ignorespaces\psi_{*}}Ω∗\scriptstyle{\lx@inpgf@ignorespaces\Omega_{*}}

commutes. This boils down to the fact that the map S1∧S1→flipS1∧S1S^{1}\wedge S^{1}\xrightarrow{\operatorname{flip}}S^{1}\wedge S^{1} has degree −1-1.

∎

The above claim therefore shows that the composite of the purple arrows (we are reversing the direction of the last arrow so as to compose) maps [idA]∈EclassG​(A,A)[\operatorname{id}_{A}]\in\mathrm{E}^{G}_{\mathrm{class}}(A,A) to [φ]∈EclassG​(A,B)[\varphi]\in\mathrm{E}^{G}_{\mathrm{class}}(A,B). The commutativity of Equation 6.7 now tells that

∂4(TA′​([idA]))=TB′​([φ]).\partial_{4}(T_{A}^{\prime}([\operatorname{id}_{A}]))=T_{B}^{\prime}([\varphi]).

Since TA′​([idA])T_{A}^{\prime}([\operatorname{id}_{A}]) is given to be dd, the proof of the proposition follows. ∎

Remark 6.7.

In the above proof, (2,2)(2,2)-periodicity played a crucial role. It would indeed be natural to expect that the same could be done by the more standard (1,1)(1,1)-periodicity. Unraveling the proof of Section 6.2, one would then want to take

EclassG​(A,B)=[[ℝ1,0​A⊗𝒦G,ℝ1,0​B⊗𝒦G]].\mathrm{E}^{G}_{\mathrm{class}}(A,B)=[[\mathbb{R}^{1,0}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{1,0}B\otimes{\mathcal{K}_{G}}]].

But it is not clear why this definition coincides with [[ℝ0,1​A⊗𝒦G,ℝ0,1​B⊗𝒦G]][[\mathbb{R}^{0,1}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{0,1}B\otimes{\mathcal{K}_{G}}]]: the results of Section 6.2 do not say this! Tracing further back, the reader may wonder “why not define EclassG​(A,B):=[[ℝ1,0​A⊗𝒦G,ℝ1,0​B⊗𝒦G]]\mathrm{E}^{G}_{\mathrm{class}}(A,B):=[[\mathbb{R}^{1,0}A\otimes{\mathcal{K}_{G}},\mathbb{R}^{1,0}B\otimes{\mathcal{K}_{G}}]]?” The reason is that then it would not be clear why this category has excision; the development of the excision results in EE-theory and the Connes-Higson morphism depend on Puppe sequences, where the loops are C0​(ℝ0,1)C_{0}(\mathbb{R}^{0,1}) and not C0​(ℝ1,0)C_{0}(\mathbb{R}^{1,0}).

Proof of Theorem 6.4.

With Section 6.2 at our disposal, the argument now follows by standard yoga with the uniqueness of the natural transformations described in loc.​ cit.​ See for example [33, Theorem 4.5]. A few more details on a similar line of ideas is in [59, Theorem 4.9]. ∎

We can now compare KKex,0G,sep\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{ex},0} with EclassGE^{G}_{\operatorname{class}}.

Theorem 6.8.

We have a natural equivalence of additive, symmetric monoidal categories

KKex,0G,sep≃EclassG.\mathrm{KK}^{G,\mathrm{sep}}_{\mathrm{ex},0}\simeq\mathrm{E}^{G}_{\mathrm{class}}.
Proof.

The proof of Theorem 6.2 can be readily adapted to this case. The main check one needs to make is that EclassG\mathrm{E}^{G}_{\mathrm{class}} has countable coproducts, and the functor EclassG\mathrm{E}^{G}_{\mathrm{class}} takes countable direct sums in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} to countable coproducts in EclassG\mathrm{E}^{G}_{\mathrm{class}}. But this is the content of [29, Proposition 7.1]. The Real structure poses no additional difficulty. ∎

6.3 A technical result of Dadarlat-Loring

In this subsection, we prove the following technical result, which will be handy in the later subsections when we study graded EE-theory. The complex, non-equivariant case of the result is due to Dadarlat-Loring ([24])

Theorem 6.9.

(Generalized Dadarlat-Loring) Let A∈𝖦𝖢∗​𝖠𝗅𝗀sepA\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}. Suppose that for all B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} the abelian monoid

homS𝒦G​AsyG⁡(A,B)=[[A⊗𝒦G,B⊗𝒦G]]\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(A,B)=[[A\otimes{\mathcal{K}_{G}},B\otimes{\mathcal{K}_{G}}]]

is a group. Then, the map

Ω:[[A⊗𝒦G,B⊗𝒦G]]→EclassG​(A,B)\Omega:[[A\otimes{\mathcal{K}_{G}},B\otimes{\mathcal{K}_{G}}]]\rightarrow\mathrm{E}^{G}_{\mathrm{class}}(A,B)

is an isomorphism of abelian groups for all B∈𝖦𝖢∗​𝖠𝗅𝗀sepB\in\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

Remark 6.9.

An AA in 𝖦𝖢∗​𝖠𝗅𝗀sep\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} satisfying the hypothesis of the above theorem is called homotopy symmetric. Note that it is equivalent to asking that the abelian monoid [[A⊗𝒦G,A⊗𝒦G]][[A\otimes{\mathcal{K}_{G}},A\otimes{\mathcal{K}_{G}}]] is a group.

Our proof strategy will be very different from [24], except that we too use Section 6.2 in a crucial way. We begin by proving the following result, wherein we use the notation from the last subsection, especially Section 6.2.

Proposition 6.9.

For each homotopy symmetric A∈S𝒦G​AsyGA\in\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}, the functor

homS𝒦G​AsyG⁡(A,−):S𝒦G​AsyG→Ab\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(A,-):\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}\rightarrow\operatorname{Ab}

inverts α:C0​(ℝ1,1)⇢𝒦⁡(l2)\alpha:C_{0}(\mathbb{R}^{1,1})\dashrightarrow\mathcal{K}(l^{2}).

Proof.

In light of Section 6.2 and the universal property of K​KKasGKK^{G}_{\operatorname{Kas}}, there is a unique dashed arrow rendering the below diagram commutative.

𝖦𝖢∗​𝖠𝗅𝗀sep{\lx@inpgf@ignorespaces{\mathsf{G}\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}}}}S𝒦G​AsyG{\lx@inpgf@ignorespaces{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}}Ab{\lx@inpgf@ignorespaces{\operatorname{Ab}}}KKKasG,sep{\lx@inpgf@ignorespaces{\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}}}kkKasG,sep\scriptstyle{\lx@inpgf@ignorespaces\mathrm{kk}_{\mathrm{Kas}}^{G,\mathrm{sep}}}homS𝒦G​AsyG⁡(A,−)\scriptstyle{\lx@inpgf@ignorespaces\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(A,-)} (6.10)

We now momentarily ignore the external group GG. Since KKKassep\mathrm{KK}_{\mathrm{Kas}}^{\mathrm{sep}} satisfies (1,1)(1,1)-periodicity, we know in light of the Cuntz picture of KKKassep\mathrm{KK}_{\mathrm{Kas}}^{\mathrm{sep}} that there is a morphism q​ℂ→𝛽C0​(ℝ1,1)⊗𝒦⁡(l2)q\mathbb{C}\xrightarrow{\beta}C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}) in 𝖢∗​𝖠𝗅𝗀sep\mathsf{C}^{*}\!\mathsf{Alg}^{\mathrm{sep}} which implements the (1,1)(1,1)-periodicity. There is also a homomorphism q​ℂ→𝛾𝒦q\mathbb{C}\xrightarrow{\gamma}\mathcal{K} given by the composite

q​ℂ→π1ℂ→𝜄𝒦⁡(l2).q\mathbb{C}\xrightarrow{\pi_{1}}\mathbb{C}\xrightarrow{\iota}\mathcal{K}(l^{2}).

We now claim the following.

Claim.

The diagram

q​ℂ{\lx@inpgf@ignorespaces{q\mathbb{C}}}𝒦⁡(l2​ℕ){\lx@inpgf@ignorespaces{\mathcal{K}(l^{2}\mathbb{N})}}C0​(ℝ1,1)⊗𝒦⁡(l2​ℕ){\lx@inpgf@ignorespaces{C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N})}}γ\scriptstyle{\lx@inpgf@ignorespaces\gamma}β\scriptstyle{\lx@inpgf@ignorespaces\beta}α\scriptstyle{\lx@inpgf@ignorespaces\alpha} (6.11)

commutes upto a sign in the 𝒦⁡(l2​ℕ)\mathcal{K}(l^{2}\mathbb{N})-stabilized asymptotic homotopy category L𝒦​AsyL_{\mathcal{K}}\!\operatorname{Asy}.

Proof.

We consider the following diagram, where the vertical maps are induced by the localization functor L𝒦​Asy→EclassL_{\mathcal{K}}\!\operatorname{Asy}\rightarrow E_{\operatorname{class}} (i.e. the trivial group case of Section 6.2).

[[q​ℂ,C0​(ℝ1,1)⊗𝒦⁡(l2​ℕ)]]×[[C0​(ℝ1,1)⊗𝒦⁡(l2​ℕ),𝒦⁡(l2​ℕ)]]⟶[[q​ℂ,𝒦⁡(l2​ℕ)]]≅ℤ↓↓↓⁣≅Eclass​(q​ℂ,C0​(ℝ1,1)⊗𝒦⁡(l2​ℕ))×Eclass​(C0​(ℝ1,1)⊗𝒦⁡(l2​ℕ),𝒦⁡(l2​ℕ))⟶Eclass​(q​ℂ,𝒦⁡(l2​ℕ))≅ℤ≅ℤ≅ℤ\begin{array}[]{ccccc}[[q\mathbb{C},C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N})]]&\times&[[C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N}),\mathcal{K}(l^{2}\mathbb{N})]]&\longrightarrow&[[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]]\cong\mathbb{Z}\\[5.16663pt] \downarrow&&\downarrow&&\downarrow\scriptstyle{\cong}\\[5.16663pt] E_{\operatorname{class}}\bigl(q\mathbb{C},C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N})\bigr)&\times&E_{\operatorname{class}}\bigl(C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N}),\mathcal{K}(l^{2}\mathbb{N})\bigr)&\longrightarrow&E_{\operatorname{class}}\bigl(q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})\bigr)\cong\mathbb{Z}\\[2.15277pt] \cong\mathbb{Z}&&\cong\mathbb{Z}&&\end{array}

We now justify the isomorphisms appearing on the diagram. That [[q​ℂ,𝒦⁡(l2​ℕ)]]≅ℤ[[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]]\cong\mathbb{Z} follows from

ℤ→≅Section 2.1[q​ℂ,𝒦⁡(l2​ℕ)]→≅Section 2.1​.6[[q​ℂ,𝒦⁡(l2​ℕ)]].\mathbb{Z}\xrightarrow[\cong]{\lx@cref{creftypecap~refnum}{prop: Cuntz picture k-theory}}[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]\xrightarrow[\cong]{\lx@cref{creftypecap~refnum}{rem: qA properties}.6}[[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]].

We furthermore note that γ\gamma corresponds to 11 under this isomorphism; see Section 2.1. The isomorphisms in the bottom row follow since q​ℂ,𝒦⁡(l2​ℕ),C0​(ℝ1,1)q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N}),C_{0}(\mathbb{R}^{1,1}) are all K​KKassepKK_{\operatorname{Kas}}^{\operatorname{sep}}-equivalent to ℂ\mathbb{C}, and K0​(ℂ)≅ℤK_{0}(\mathbb{C})\cong\mathbb{Z}. That the right vertical map is an isomorphism follows from the composite map

[q​ℂ,𝒦⁡(l2​ℕ)]→≅[[q​ℂ,𝒦⁡(l2​ℕ)]]→Eclass​(ℂ,ℂ)[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]\xrightarrow{\cong}[[q\mathbb{C},\mathcal{K}(l^{2}\mathbb{N})]]\rightarrow E_{\operatorname{class}}(\mathbb{C},\mathbb{C})

being an isomorphism from Section 3.6 (we are implicitly also using the universal property of 𝒦⁡(l2)\mathcal{K}(l^{2})-stabilized homotopy category of separable C∗C^{*}-algebras here). From the discussion preceding the claim, β\beta and α\alpha map to a generator in ℤ\mathbb{Z} under the two left vertical arrows. An argument similar to the one in Section 4.1 shows that the bottom bilinear map must send 1×11\times 1 to ±1\pm 1. The conclusion follows. ∎

We are now in a position to bring back the group GG. Since all the algebras in Equation 6.11 have the trivial GG-action, we conclude that Equation 6.11 also commutes in S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}. Furthermore, γ\gamma and β\beta remain equivalences in KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}, whence so is α\alpha. The proof of the proposition follows in light of Equation 6.10. ∎

Proof of Theorem 6.9.

In light of Section 6.2 and general facts about mapping spaces (in our context, mapping abelian groups) out of colocal objects ([17, Remark 9.9]), it suffices to show that the functor

homS𝒦G​AsyG⁡(A,−):S𝒦G​AsyG→Ab\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(A,-):\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}\rightarrow\operatorname{Ab}

inverts the morphisms α⊗1B:C0​(ℝ1,1)⊗B⇢𝒦⁡(l2​ℕ)⊗B\alpha\otimes 1_{B}:C_{0}(\mathbb{R}^{1,1})\otimes B\dashrightarrow\mathcal{K}(l^{2}\mathbb{N})\otimes B. But this follows upon tensoring Equation 6.11 with BB; the diagram continues to commute up to a sign (which is independent of BB), and the morphisms q​ℂ⊗B→β⊗1BC0​(ℝ1,1)⊗𝒦⁡(l2​ℕ)⊗Bq\mathbb{C}\otimes B\xrightarrow{\beta\otimes 1_{B}}C_{0}(\mathbb{R}^{1,1})\otimes\mathcal{K}(l^{2}\mathbb{N})\otimes B and q​ℂ⊗B→γ⊗1B𝒦⁡(l2​ℕ)⊗Bq\mathbb{C}\otimes B\xrightarrow{\gamma\otimes 1_{B}}\mathcal{K}(l^{2}\mathbb{N})\otimes B are isomorphisms in KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}. ∎

Remark 6.11.

The following remarks about Theorem 6.9 are in order.

  1. 1.

    There is a non-technical way to think about the result. Note that Section 6.2 roughly says that one obtains EclassG\mathrm{E}^{G}_{\mathrm{class}} from S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G} by “inverting Bott”. When AA is homotopy symmetric, Equation 6.10 shows that the functor

    homS𝒦G​AsyG⁡(A,−):S𝒦G​AsyG→Ab\operatorname{hom}_{\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}}(A,-):\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}\rightarrow\operatorname{Ab}

    indeed “inverts Bott”, since it factors through KKKasG,sep\mathrm{KK}_{\mathrm{Kas}}^{G,\mathrm{sep}}. Section 6.3 basically makes this line of argument rigorous. And probably this is also the argument which was hinted at the end of Section 4 in [24].

  2. 2.

    A treatment analogous to Section 3.4 would now show that EclassG\mathrm{E}^{G}_{\mathrm{class}} is the full subcategory of group objects of S𝒦G​AsyG\mathrm{S}_{{\mathcal{K}_{G}}}\Asy^{G}. This seems to not have been mentioned in the literature.

6.4 Comparison with classical, graded E^G\widehat{E}^{G}-theory

We are finally in a position to discuss classical, graded E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}}-categories. The main reference for the same is [32, Section 2] (in the complex case). Following the formulation given there, we introduce its Real analogue. In what follows, [[A,B]]gr[[A,B]]_{\operatorname{gr}} denotes the homotopy classes of graded, GG-equivariant asymptotic morphisms from AA to BB. Recall that E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}} still denotes the separable theory.

Definition 6.11.

(cf. [32, Chapter 2]) For A,B∈𝖦​𝖢^∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, define a category E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}} with objects the objects of 𝖦​𝖢^∗​𝖠𝗅𝗀\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}, and morphims from AA to BB being given by

E^classG​(A,B):=[[𝒮​⊗^​A​⊗^​𝒦^G,B​⊗^​𝒦^G]]gr.\widehat{\mathrm{E}}^{G}_{\mathrm{class}}(A,B):=[[\mathcal{S}\hat{\otimes}A\hat{\otimes}\hat{\mathcal{K}}_{G},B\hat{\otimes}\hat{\mathcal{K}}_{G}]]_{\operatorname{gr}}.

The composition law in E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}} is given by the usual formula (see [32, Definition 2.9]) using the codiagonal map 𝒮→Δ𝒮​⊗^​𝒮\mathcal{S}\xrightarrow{\Delta}\mathcal{S}\hat{\otimes}\mathcal{S}. Denote by

e^classG:𝖦​𝖢^∗​𝖠𝗅𝗀sep→E^classG\widehat{\mathrm{e}}^{G}_{\mathrm{class}}:\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}\rightarrow\widehat{\mathrm{E}}^{G}_{\mathrm{class}}

the canonical functor induced by precomposition with the homomorphism 𝒮→ev0ℂ\mathcal{S}\xrightarrow{\operatorname{ev}_{0}}\mathbb{C}.

To connect E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}} and KK^ex,0G,sep\widehat{\mathrm{KK}}_{\mathrm{ex},0}^{G,\mathrm{sep}}, we need the following lemma.

Lemma 6.11.

The abelian monoid [[𝒮​⊗^​A​⊗^​𝒦^G,B​⊗^​𝒦^G]]gr[[\mathcal{S}\hat{\otimes}A\hat{\otimes}\hat{\mathcal{K}}_{G},B\hat{\otimes}\hat{\mathcal{K}}_{G}]]_{\operatorname{gr}} is a group for all A,B∈𝖦​𝖢^∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}.

Proof.

This follows from an argument very similar to the argument given in the proof of Theorem 2.3.1. See [32, Lemma 2.1] for more details. ∎

Theorem 6.12.
  1. 1.

    For all A,B∈𝖦​𝖢^∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we have a natural isomorphism EclassG2​(𝒮​⊗^​A,B)≅E^classG​(A,B)\mathrm{E}^{G_{2}}_{\mathrm{class}}(\mathcal{S}\hat{\otimes}A,B)\cong\widehat{\mathrm{E}}^{G}_{\mathrm{class}}(A,B).

  2. 2.

    We have an equivalence of additive, symmetric monoidal (for the graded maximal tensor product) categories

    KK^ex,0G,sep≃E^classG.\widehat{\mathrm{KK}}_{\mathrm{ex},0}^{G,\mathrm{sep}}\simeq\widehat{\mathrm{E}}^{G}_{\mathrm{class}}.
  3. 3.

    For ungraded C∗C^{*}-algebras AA and BB in 𝖦​𝖢^∗​𝖠𝗅𝗀sep\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}}, we have a natural isomorphism

    E^classG​(A,B)≅EclassG​(A,B).\widehat{\mathrm{E}}^{G}_{\mathrm{class}}(A,B)\cong\mathrm{E}^{G}_{\mathrm{class}}(A,B).
Proof.

Assertion 1 follows immediately from Theorem 6.9 and Section 6.4, keeping in mind that 𝒦^G\hat{\mathcal{K}}_{G} is inner graded. Assertion 2 follows from Theorem 6.8 for the group G×C2G\times C_{2} (with the monoidal structure being the graded maximal tensor product), Assertion 1, and Section 4.5. Assertion 3 was shown in the context of our stable ∞\infty-categories in Theorem 4.2. We are therefore done by Assertion 2. ∎

We end the article with a remark circling the analogous comparison between K​K^KasG,sep\widehat{KK}_{\operatorname{Kas}}^{G,\operatorname{sep}} and KK^se,0G,sep\widehat{\mathrm{KK}}_{\mathrm{se},0}^{G,\mathrm{sep}}.

Remark 6.12.

In light of the main result of [59], we can rework the last two subsections with completely positive asymptotic morphisms, and obtain that for all A,B∈𝖦​𝖢^∗​𝖠𝗅𝗀sepA,B\in\mathsf{G}\widehat{\mathsf{C}}^{*}\!\mathsf{Alg}^{\mathrm{sep}},

KK^se,0G,sep​(A,B)≅[[𝒮​⊗^​A​⊗^​𝒦^G,B​⊗^​𝒦^G]]grcp.\widehat{\mathrm{KK}}_{\mathrm{se},0}^{G,\mathrm{sep}}(A,B)\cong[[\mathcal{S}\hat{\otimes}A\hat{\otimes}\hat{\mathcal{K}}_{G},B\hat{\otimes}\hat{\mathcal{K}}_{G}]]_{\operatorname{gr}}^{\operatorname{cp}}.

However, unlike the definition of E^classG\widehat{\mathrm{E}}^{G}_{\mathrm{class}} (which on the face of it is by asymptotic morphisms), the definition of KK^KasG,sep\widehat{\mathrm{KK}}_{\mathrm{Kas}}^{G,\mathrm{sep}} is in terms of Kasparov cycles. Therefore to complete the circle of ideas, we would need to obtain a natural isomorphism

KK^KasG,sep​(A,B)≅[[𝒮​⊗^​A​⊗^​𝒦^G,B​⊗^​𝒦^G]]grcp.\widehat{\mathrm{KK}}_{\mathrm{Kas}}^{G,\mathrm{sep}}(A,B)\cong[[\mathcal{S}\hat{\otimes}A\hat{\otimes}\hat{\mathcal{K}}_{G},B\hat{\otimes}\hat{\mathcal{K}}_{G}]]_{\operatorname{gr}}^{\operatorname{cp}}.

It is not clear to the author how to get a (clean) natural map in either direction. The problem seems to be that completely positive asymptotic morphisms do not naturally arise in practical situations.

Nevertheless, Meyer has proven using different methods in [46, Section 7] the analogue of the first two assertions of Theorem 6.12 for K​K^KasG,sep\widehat{KK}_{\operatorname{Kas}}^{G,\operatorname{sep}}, whence the analogue of Assertion 3 of Theorem 6.12 for KK^KasG,sep\widehat{\mathrm{KK}}_{\mathrm{Kas}}^{G,\mathrm{sep}} also follows from Theorem 4.2.

References