ScalingStacks

2.2. The ∞\infty-categories Cat∞ex\Cat_{\infty}^{\ex} and Cat∞perf\Cat_{\infty}^{\perf}

The basic setting for our work is the theory of ∞\infty-categories (and particularly stable ∞\infty-categories), which provide a tractable way to handle a “homotopical category of homotopical categories” as well as homotopically meaningful categories of homotopical functors. There are now many competing models of ∞\infty-categories, including Rezk’s complete Segal spaces [77], the Segal categories [43, 78] of Simpson and Tamsamani, the quasicategories (weak Kan complexes) of Boardman and Vogt, the homotopy theory of simplicial categories as studied by Dwyer-Kan and Bergner  [28, 6], and others, all of which are known to be equivalent (see [7] for a nice discussion of the situation). In a sense the situation is analogous to the situation with the varied modern categories of spectra (e.g., symmetric spectra, orthogonal spectra, EKMM SS-modules). None of the work of this paper depends in any way on particular properties of the model of ∞\infty-categories chosen; given certain basic structural properties, one could carry out our arguments in any of them.

We have chosen to work in this paper with the theory of quasicategories. These first appeared in the work of Boardman and Vogt, where they were referred to as weak Kan complexes [15]. The theory was subsequently developed by Joyal [46] and then extensively studied by Lurie. In this section we give a rapid review of the relevant background on the theory of quasicategories as a model of ∞\infty-categories. Our basic references for this material are Lurie’s books [52, 53].

We will write Cat∞\Cat_{\infty} to denote the ∞\infty-category of small ∞\infty-categories and functors, which we explicitly model as the category of simplicial sets with the Joyal model structure [46]. There is a simplicial nerve functor N\mathrm{N} from simplicial categories to simplicial sets which is the right Quillen functor of a Quillen equivalence [52, §1.1.5.5, 1.1.5.13, 2.2.5.1]

Cat𝒯\textstyle{\Cat_{\mathcal{T}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N\scriptstyle{N}SetΔ.\textstyle{\Set_{\Delta}\ignorespaces\ignorespaces\ignorespaces\ignorespaces.}ℭ\scriptstyle{\mathfrak{C}}

Here the model structure on the top is Bergner-Dwyer-Kan’s model structure on simplicial categories [6] and the model structure on the bottom is Joyal’s model structure on simplicial sets.

There are a number of options for producing the “underlying” ∞\infty-category of a category equipped with a notion of “weak equivalence”. The most structured setting is that of a simplicial model category 𝒞{\mathcal{C}}, where the ∞\infty-category can be obtained by restricting to the full simplicial subcategory 𝒞cf{\mathcal{C}}^{\cf} of cofibrant-fibrant objects and then applying the simplicial nerve functor N\mathrm{N}. More generally, if 𝒞{\mathcal{C}} is a category equipped with a subcategory of weak equivalences w​𝒞w{\mathcal{C}}, the Dwyer-Kan simplicial localization L​𝒞L{\mathcal{C}} [28] provides a corresponding simplicial category, and then N⁡((L​𝒞)fib)\mathrm{N}((L{\mathcal{C}})^{\textrm{fib}}), where (−)fib(-)^{\textrm{fib}} denotes fibrant replacement in simplicial categories, yields an associated ∞\infty-category. Barwick and Kan [4] have studied this procedure in the context of Segal spaces and Lurie has given a version of this approach in [53, §1.3.3]: we associate to a (not necessarily simplicial) category 𝒞{\mathcal{C}} with weak equivalences WW an ∞\infty-category N​(𝒞)​[W−1]\mathrm{N}({\mathcal{C}})[W^{-1}]; when 𝒞{\mathcal{C}} is a model category, for functoriality reasons it is usually convenient to restrict to the cofibrant objects 𝒞c{\mathcal{C}}^{\mathrm{c}} and consider N⁡(𝒞c)​[W−1]\mathrm{N}({\mathcal{C}}^{\mathrm{c}})[W^{-1}].

All of these constructions produce equivalent ∞\infty-categories [53, 1.3.7]. Furthermore, all of them are functorial. Although a simplicial left Quillen functor 𝒞→𝒟{\mathcal{C}}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}{\mathcal{D}} does not typically induce a functor between the subcategories of cofibrant-fibrant objects in 𝒞{\mathcal{C}} and 𝒟{\mathcal{D}} respectively, composing with a fibrant replacement functor as in definition 2.7, does yield an induced functor on simplicial nerves. Furthermore, given a simplicial Quillen adjunction (F,G)(F,G), there is an induced adjunction of functors on the level of ∞\infty-categories by [52, 5.2.4.6]. (Alternatively, it can be seen directly that a functor 𝒞→𝒟{\mathcal{C}}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}{\mathcal{D}} which preserves weak equivalences between cofibrant objects induces a functor N⁡(𝒞)​[W−1]→N⁡(𝒟)​[W−1]\mathrm{N}({\mathcal{C}})[W^{-1}]\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\mathrm{N}({\mathcal{D}})[W^{-1}].)

Given an ∞\infty-category 𝒞{\mathcal{C}}, we can form its homotopy category Ho⁡(𝒞)\Ho({\mathcal{C}}), which is an ordinary category [52, §1.2.3]. In addition, given an ∞\infty-category 𝒞{\mathcal{C}}, there is a maximal ∞\infty-groupoid (Kan complex) 𝒞iso{\mathcal{C}}_{\mathrm{iso}} inside of 𝒞{\mathcal{C}}, obtained by restricting to the subcategory of 𝒞{\mathcal{C}} consisting of those arrows which become isomorphisms in the homotopy category Ho⁡(𝒞)\Ho({\mathcal{C}}). The functor which associates to the ∞\infty-category 𝒞{\mathcal{C}} its maximal subgroupoid 𝒞iso{\mathcal{C}}_{\mathrm{iso}} is right adjoint to the inclusion of ∞\infty-groupoids into ∞\infty-categories. We have the following proposition relating this to other, possibly more familiar, notions (see also [81, 2.3]).

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Proposition 2.10. Let 𝒞{\mathcal{C}} be a small category with a subcategory w​𝒞w{\mathcal{C}} of weak equivalences which satisfies a homotopy calculus of two-sided fractions (in the sense of Dwyer and Kan [29, 6.1]). Then there is a weak equivalence of simplicial sets

N⁡(w​𝒞)≃(N⁡((LH​𝒞)fib))iso,\mathrm{N}(w{\mathcal{C}})\simeq(\mathrm{N}((L^{H}{\mathcal{C}})^{\mathrm{fib}}))_{\mathrm{iso}},

where here LH​𝒞L^{H}{\mathcal{C}} denotes the hammock version of the simplicial localization [29] and (LH​𝒞)fib(L^{H}{\mathcal{C}})^{\mathrm{fib}} is a fibrant replacement of LH​𝒞L^{H}{\mathcal{C}} as a simplicial category.

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Proof. There is an “inclusion” functor 𝒞→LH​𝒞{\mathcal{C}}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}L^{H}{\mathcal{C}}. Restricting to the weak equivalences and passing to nerves via N\mathrm{N}, we obtain a map of simplicial sets

(2.11) N⁡(w​𝒞)⟶N⁡(LH​w​𝒞)⟶N⁡((LH​w​𝒞)fib);\mathrm{N}(w{\mathcal{C}})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\mathrm{N}(L^{H}w{\mathcal{C}})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\mathrm{N}((L^{H}w{\mathcal{C}})^{\mathrm{fib}});

note that the nerve of w​𝒞w{\mathcal{C}} is the same whether we regard it as a category or as a category (trivially) enriched in simplicial sets [52, 1.1.5.8]. Since (N⁡((LH​w​𝒞)fib))iso(\mathrm{N}((L^{H}w{\mathcal{C}})^{\mathrm{fib}}))_{\mathrm{iso}} is isomorphic to N⁡((LH​w​𝒞)fib)\mathrm{N}((L^{H}w{\mathcal{C}})^{\mathrm{fib}}), the inclusion LH​w​𝒞→LH​𝒞L^{H}w{\mathcal{C}}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}L^{H}{\mathcal{C}} induces a natural map N⁡((LH​w​𝒞)fib)→(N⁡((LH​𝒞)fib))iso\mathrm{N}((L^{H}w{\mathcal{C}})^{\mathrm{fib}})\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}(\mathrm{N}((L^{H}{\mathcal{C}})^{\mathrm{fib}}))_{\mathrm{iso}}; under the hypothesis that 𝒞{\mathcal{C}} satisfies a homotopy calculus of fractions, this map is a weak equivalence [29, 6.4]. Therefore, it suffices to show that the map of equation 2.11 is a weak equivalence. We consider the map on components; for each homotopy equivalence class [x][x], both sides are equivalent to B​haut⁡(x)B\haut(x) and it is straightforward to see that the map induces the equivalence. ∎

The ∞\infty-category of functors between two ∞\infty-categories 𝒞{\mathcal{C}} and 𝒟{\mathcal{D}} is denoted Fun⁡(𝒞,𝒟)\mathrm{Fun}({\mathcal{C}},{\mathcal{D}}). As a point-set object, in this setting Fun⁡(𝒞,𝒟)\mathrm{Fun}({\mathcal{C}},{\mathcal{D}}) is the simplicial set of maps between the quasicategories 𝒞{\mathcal{C}} and 𝒟{\mathcal{D}}, which is itself a quasicategory. Note that the space of functors from 𝒞{\mathcal{C}} to 𝒟{\mathcal{D}} is precisely the maximal subgroupoid Fun​(𝒞,𝒟)iso\mathrm{Fun}({\mathcal{C}},{\mathcal{D}})_{\mathrm{iso}} of Fun⁡(𝒞,𝒟)\mathrm{Fun}({\mathcal{C}},{\mathcal{D}}) [52, 1.2.5.3, 3.0.0.1].

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Definition 2.12. An ∞\infty-category is stable [53, 1.1.1.9] if it has finite limits and colimits and pushout and pullback squares coincide [53, 1.1.3.4]. Let Cat∞ex\Cat_{\infty}^{\ex} denote the (pointed) ∞\infty-category of small stable ∞\infty-categories and exact functors (i.e., functors which preserve finite limits and colimits) [53, §1.1.4]. The ∞\infty-category of exact functors between 𝒜{\mathcal{A}} and ℬ{\mathcal{B}} is denoted by Funex​(𝒜,ℬ)\mathrm{Fun}^{\ex}({\mathcal{A}},{\mathcal{B}}); this is the full ∞\infty-subcategory of Fun⁡(𝒜,ℬ)\mathrm{Fun}({\mathcal{A}},{\mathcal{B}}) spanned by the exact functors.

For a small stable ∞\infty-category 𝒞{\mathcal{C}}, the homotopy category Ho⁡(𝒞)\Ho({\mathcal{C}}) is triangulated, with the exact triangles determined by the cofiber sequences in 𝒞{\mathcal{C}} [53, 1.1.2.13].

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Remark 2.13. A small stable ∞\infty-category corresponds to the notion of a pretriangulated spectral category, and the weak equivalences are given by exact functors which induce triangulated equivalences on passage to the homotopy category. We will make this correspondence precise in section 4, but for now observe that given a pretriangulated spectral category 𝒞{\mathcal{C}}, the ∞\infty-category N⁡((Mod⁡(𝒞))cf)\mathrm{N}((\mathrm{Mod}({\mathcal{C}}))^{\cf}) is stable. Recall that a stable model category is a pointed model category 𝒞{\mathcal{C}} for which the functors Σ\Sigma and Ω\Omega on Ho⁡(𝒞)\Ho({\mathcal{C}}) are inverse equivalences. Given a stable simplicial model category 𝒞{\mathcal{C}}, the ∞\infty-category N⁡(𝒞cf)\mathrm{N}({\mathcal{C}}^{\cf}) is stable. More generally, if 𝒞{\mathcal{C}} is a stable model category, N⁡(𝒞c)​[W−1]\mathrm{N}({\mathcal{C}}^{\mathrm{c}})[W^{-1}] is a stable ∞\infty-category.

Recall that an ∞\infty-category 𝒞{\mathcal{C}} is idempotent-complete if the image of 𝒞{\mathcal{C}} under the Yoneda embedding 𝒞→Pre⁡(𝒞){\mathcal{C}}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\mathrm{Pre}({\mathcal{C}}) is closed under retracts (see also [52, §4.4.5]); here Pre⁡(𝒞)\mathrm{Pre}({\mathcal{C}}) denotes the ∞\infty-category Fun⁡(𝒞op,N⁡(𝒯cf))\mathrm{Fun}({\mathcal{C}}^{\op},\mathrm{N}({\mathcal{T}}^{\cf})) of presheaves of spaces on 𝒞{\mathcal{C}}. Let Cat∞perf\Cat_{\infty}^{\perf} denote the ∞\infty-category of small idempotent-complete stable ∞\infty-categories. There is an idempotent completion functor given as the left adjoint to the inclusion Cat∞perf→Cat∞ex\Cat_{\infty}^{\perf}\mathchoice{\longrightarrow}{\rightarrow}{\rightarrow}{\rightarrow}\Cat_{\infty}^{\ex} [52, 5.1.4.2], which we denote by Idem\Idem.

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Definition 2.14. Let 𝒜{\mathcal{A}} and ℬ{\mathcal{B}} be small stable ∞\infty-categories. Then we will say that 𝒜{\mathcal{A}} and ℬ{\mathcal{B}} are Morita equivalent if Idem⁡(𝒜)\Idem({\mathcal{A}}) and Idem⁡(ℬ)\Idem({\mathcal{B}}) are equivalent.

We will verify shortly that this notion of Morita equivalence is compatible with the definition given in terms of spectral categories in definition 2.7.

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Andrew J. Blumberg, David Gepner, Goncalo Tabuada

Original source: arXiv:1001.2282v4