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Grothendieck’s by inspired -categories -groupoid n ′ F hc ilntb smrhcto isomorphic be not will which , ntrso the of terms in , coherator n 55P15 Introduction ( i aso soitn oafiiefamily finite a to associating of ways ∞ ) ujce oa“tnad e frltoson relations of set “standard” a to subjected , ctgr,hmtp ye ekfcoiainsystem. factorization weak type, homotopy -category, , 83,18B40, 18A30, 55Q05 1 ( F category , ntesneo r X Mr. of sense the in ∞ ∞ ihstof set with , gopis[,scin -3 a been has 1-13] sections [5, -groupoids -GROUPOIDS, 53,55U40. 55U35, , ∞ ∞ gopi tutr ny then only, structure -groupoid C C ogl aig w different two saying, Roughly gopi speetda fol- as presented is -groupoid 18C10 ∞ noe iha“universal a with endowed aifigsm etexact- left some satisfying i ctgre 8,vr close very [8], -categories ∞ -cells hsabgiyhowever ambiguity this eoisof tegories -CATEGORIES 83,18C35, 18C30, , olmIhdi mind, in had I roblem h eysrcueof structure very the n n fM.Yand Y Mr. of one X . lotcranyget certainly almost l ∞ n u uco or functor a out ink F orcnieM.X Mr. reconcile to 5 eto 9]. section [5, ” . . . gopis Never- -groupoids. ) i :“ ): lascaet a to associate ll T T ae ihthe with faced , ∞ ≃ fcus,but course, of nparticular, In nutvl,it Intuitively, dto nd T ( set-valued, ′ ( n the and , eetwo hese u i 18D05 ) i ∈ I no- ry of , 2 GEORGES MALTSINIOTIS and Mr. Y, which very probably won’t be equivalent (I mean isomorphic) to the previous one. Here however a fifth mathematician, informed about this new per- plexity, will probably show that the two Y -structures U and U ′, associated by his two colleagues to an X-structure T , while not isomorphic, also admit however a canonical ∞-equivalence between U and U ′ (in the sense of the Y -theory). I could go on with a sixth mathematician, confronted with the same perplexity as the previ- ous one, who winds up with another ∞-equivalence between U and U ′ (without being informed of the work of the fifth), and a seventh reconciling them by discovering an ∞-equivalence between these equivalences. The story of course is infinite, I better stop with seven mathematicians, . . . ” [5, section 9]. One of the reasons of Grothendieck’s interest in ∞-groupoids is that (weak) ∞-groupoids are conjectured to modelize homotopy types (it’s well known that strict ∞-groupoids don’t): “Among the things to be checked is of course that when we localize the category of ∞-groupoids with respect to morphisms which are “weak equivalences” in a rather obvious sense (N.B. – the definition of the πi’s of an ∞-groupoid is practically trivial!), we get a category equivalent to the usual ho- motopy category Hot.” [5, section 12]. This conjecture is still not proven, for any definition of ∞-groupoid giving rise to an algebraic structure species, although some progress has been done in this direction by Cisinski [4]. It becomes tautological if we define ∞-groupoids as being Kan complexes or topological spaces! But the cat- egories of such are not locally presentable. In a letter to Tim Porter, Grothendieck clearly explains that this was not the kind of definition he was looking for: “my main point is that your suggestion that Kan complexes are “the ultimate in lax ∞-groupoids” does not in any way meet with what I am really looking for, and this for a variety of reasons, . . . ”[6]. One of the peculiarities of Grothendieck’s definition of ∞-groupoids is that this notion is not a particular case of a concept of lax ∞-category. Nevertheless, it was realized in [8] that a slight modification of the notion of coherator gives rise to such a concept. This new formalization of lax ∞-categories is very close, although not exactly equivalent, to the notion introduced by Batanin [2]. From a technical point of view, the basic difference is that the first is based on universal algebra, whereas the second on a generalization of the notion of operads, the globular operads. The precise relationship between the two concepts is studied in [1]. In the first section, Grothendieck’s definition of ∞-groupoids is presented (in a two-page slightly simplified form), introducing the notion of “coherator for a theory of ∞-groupoids”. Some examples of such coherators are given. The aim of the very long (too long?) last subsection 1.7 is to convince the reader of the pertinence of Grothendieck’s concept, and define some structural maps in ∞-groupoids, useful in the next section. In section 2, homotopy groups and weak equivalences between ∞-groupoids are introduced. The pair of adjoint functors “classifying space” of a ∞-groupoid and “fundamental ∞-groupoid” of a topological space are defined. Grothendieck’s con- jecture is presented. In section 3, the only really original part of this paper, an interpretation of the notion of coherator for a theory of ∞-groupoids, in terms of lifting properties and weak factorization systems, is given. In the last section, the definition of ∞-categories of [8] is presented, introducing the notion of “coherator for a theory of ∞-categories”. The reader mainly interested by this definition can read directly this section after 1.4 and skip everything in between. In appendix A, a technical result used in section 3 is proved. GROTHENDIECK ∞-GROUPOIDS, AND A DEFINITION OF LAX ∞-CATEGORIES 3
1. Grothendieck ∞-groupoids 1.1. The category of globes. The globular category or category of globes is the category G generated by the graph
σ σ σ − σ σ 1 / 2 / i 1 / i / i+1 / D0 / D1 / / Di−1 / Di / , τ 1 τ 2 τ i−1 τ i τ i+1 under the coglobular relations
σi+1σi = τ i+1σi and σi+1τ i = τ i+1τ i , i > 1 . For every i, j, such that 0 6 i 6 j, define j j σi = σj σi+2σi+1 and τ i = τ j τ i+2τ i+1 , and observe that j j {σi , τ i } , if i < j , HomG(Di, Dj )= {1 } , if i = j , Di ∅ , else. G / 1.2. Globular sums. Let C be a category, C a functor, and let Di, σi, τi, j j j j σi , τi be the image in C of Di, σi, τ i, σi , τ i respectively. A standard iterated amalgamated sum, or more simply a globular sum, of length m, in C is an iterated amalgamated sum of the form
i1 i2 i2 im (Di , σ ′ ) ∐ ′ (τ ′ ,Di , σ ′ ) ∐ ′ ∐ ′ (τ ′ ,Di ) , 1 i Di i 2 i Di Di i − m 1 1 1 2 2 m−1 m 1 colimit of the diagram
D D D D − D i1 _ ? i2 _ ? i3 im 1 < im @@ ~ @@ ~ Hc H y @@ ~~ @@ ~~ HH yy i1 @ ~ i2 i2 @ ~ i3 im−1 HH yy im σ ′ ~ τ ′ σ ′ ~ τ ′ σ ′ y τ ′ i i i ′ i i i − 1 ′ 1 2 ′ 2 m−1 ′ m 1 , Di D Di − 1 i2 m 1 ′ where m > 1, and for every k, 1 6 k