The language of higher category theory in more than analogous to homotopy theory, especially in the cellular version. What is the appropriate reference for a non-categorical reader? Have the A_\infty categories of Smirnov or Fukaya been treated in the categorical literature?? thanks .oooO Jim Stasheff jds@math.unc.edu (UNC) Math-UNC (919)-962-9607 \ ( Chapel Hill NC FAX:(919)-962-2568 \*) 27599-3250 http://www.math.unc.edu/Faculty/jds
Jim Stasheff writes:
The language of higher category theory in more than analogous to homotopy theory, especially in the cellular version. What is the appropriate reference for a non-categorical reader? Have the A_\infty categories of Smirnov or Fukaya been treated in the categorical literature??
Unfortunately the truly appropriate reference has not yet been written, because the equivalence between weak infinity-groupoids and homotopy types has not yet worked out in full detail, at least not in the cellular version. The *dream* of translating all of homotopy theory into higher category theory is outlined in: John Baez and James Dolan, Categorification, to appear in Proceedings Workshop on Higher Category Theory and Mathematical Physics at Northwestern University, Evanston, Illinois, March 1997, eds. Ezra Getzler and Mikhail Kapranov, preprint available as math.QA/9802029. This also has lots of references to different places where various bits of the dream have been realized. Basically the dream consists of working out the following correspondence: HIGHER CATEGORY THEORY HOMOTOPY THEORY omega-groupoids homotopy types n-groupoids homotopy n-types k-tuply groupal omega-groupoids homotopy types of k-fold loop spaces k-tuply groupal n-groupoids homotopy n-types of k-fold loop spaces k-tuply monoidal omega-groupoids homotopy types of E_k spaces k-tuply monoidal n-groupoids homotopy n-types of E_k spaces stable omega-groupoids homotopy types of infinite loop spaces stable n-groupoids homotopy n-types of infinite loop spaces Z-groupoids homotopy types of spectra How do A_infinity categories fit in? As far as I can tell they should correspond to omega-categories where all j-morphisms are invertible for j > 1.
The language of higher category theory in more than analogous to homotopy theory, especially in the cellular version. What is the appropriate reference for a non-categorical reader? Have the A_\infty categories of Smirnov or Fukaya been treated in the categorical literature??
Fortunately, since the A_\infty categories (described sketchily in the preprint I have of Fukaya) use chain complexes rather than topological spaces (so that I believe a 1-object A_\infty category is an algebra for the A_\infty non-permutative operad on chain complexes - an A_\infty DG-algebra), we do not need to realise the whole homotopy types dream (as described by John Baez) to give a categorical description of A_\infty categories. Several years ago I remember discussing this by email with Jim Stasheff. Dominic Verity was here at the time. I cannot remember all the details but the two basic ingredients were some free strict n-categories made from the set (whose elements are to be the objects of the A_\infty category) in much the way the orientals are constructed, and the construction (below) mentioned in my Oberwolfach Descent Theory notes of September 1995. There is a connection between the Gray tensor product and ordinary chain complexes. Each chain complex R gives rise to a (strict) omega-category J(R) whose 0-cells are 0-cycles a in R, whose 1-cells b : a --> a' are elements b in R_1 with d(b) = a'- a, whose 2-cells c : b --> b' are elements c in R_2 with d(c) = b'- b, and so on. All compositions are addition. This gives a functor J : DG --> omega-Cat from the category DG of chain complexes and chain maps. In fact, J : DG --> omega-Cat is a monoidal functor where DG has the usual tensor product of chain complexes and omega-Cat has the Gray tensor product. By applying J on homs, we obtain a (2-) functor J_* : DG-Cat --> V_2-Cat, where V_2 is omega-Cat with the Gray-like tensor product (extending the natural tensor product of oriented cubes as described in Sjoerd Crans thesis). In particular, since DG is closed, it is a DG-category and we can apply J_* to it. The V_2-category J*(DG) has chain complexes as 0-cells and chain maps as 1-cells; the 2-cells are chain homotopies and the higher cells are higher analogues of chain homotopies. Best regards, Ross
I have not seen Fukaya's paper. If the problem is to formalise higher homotopies for, say, topological spaces or chain complexes, together with their operations, there is a simple solution based on the path endofunctor (or, dually, the cylinder endofunctor; or their adjunction) and its powers. The path endofunctor P is constructed so that a homotopy a: f -> g: X -> Y amounts to a map a: X -> PY; the maps f, g are recovered by means of the two faces d-, d+: PY -> Y. (For Top, PY is obviously the space Y^[0, 1] of paths in Y, with the compact-open topology; for chain complexes (PY)_n = Y_n + Y_(n+1) + Y_n, with suitable differential.) P comes equipped with various natural transformations (faces, degeneracy, connections, symmetries, concatenation...), satisfying "algebraic" coherence axioms (a sort of "cubical comonad" with additional structure). These transformations represent the basic structure of lower order homotopies. But now you have, practically for free: - n-tuple homotopies, represented by the power endofunctor P^n, - n-homotopies, represented by a subfunctor P_n of P^n, - their operations, via the usual algebra of natural transformations, - the deduced coherence relations of the latter. Eg, a double homotopy, represented by a map X -> P^2(Y), has four faces given by the four natural transformations d-P, d+P, Pd-, Pd+: P^2 -> P; if k is the concatenation of homotopies, kP and Pk are the vertical and horizontal concatenation of double homotopies, and so on; if k is associative, as is the case for chain complexes but not for spaces, so are all higher concatenations. A double homotopy is said to be a 2-homotopy when its "vertical" faces (say) are trivial, i.e. factor through the degeneracy 1 -> P. (For Top, P^2(Y) is the space of maps from the standard square [0, 1]^2 to Y; P_2(Y) is the subspace of those maps which are constant on the vertical faces of the square.) This way of deducing higher homotopies and their operations from the lower ones can be found in: M. Grandis, Categorically algebraic foundations for homotopical algebra, Appl. Categ. Structures 5 (1997), 363-413. M. Grandis, On the homotopy structure of strongly homotopy associative algebras, J. Pure Appl. Algebra, 134 / 1 (1999 ?), 15-81. Regards, Marco Grandis Dipartimento di Matematica Universita' di Genova via Dodecaneso 35 16146 GENOVA, Italy e-mail: grandis@dima.unige.it http://pitagora.dima.unige.it/webdima/STAFF/GRANDIS/ ftp://pitagora.dima.unige.it/WWW/FTP/GRANDIS/
This is a summary of my correspondence with J.Stasheff. James Stasheff wrote:
As monoids can be described as categories with one object, one can consider \Aoo structures on categories with a notion of homotopy, e.g. topological categories or differential graded categories. To be more precise, the set of objects and the set of morphisms carry a notion of homotopy. As usual, one deals with composable morphisms and then weakens the axiom of associativity up to homotopy in the strong sense in order to define \Aoo - categories. This was first done by Smirnov by 1987 \cite{smirnov:baku} to handle functorial homology operations and their dependence on choices (cf. indeterminacy). More recently, Fukaya \cite{fukaya:1} reinvented \Aoo -categories with remarkable applications to Morse theory and Floer homology. Inspired by this work, Nest and Tsygan have proposed an \Aoo -category with automorphisms of an associative algebra as objects and for the space of morphisms, a twisted version of the Hochschild complex of the corresponding endomorphism algebras.
Michael Batanin: One can generalize "ordinary" category theory in the different ways. One can consider internal category theory, enriched category theory. We can also consider a category as a special sort of simplicial set. All this points of view have their own A_{\infty}-analogues. I realize, that the approach of Smirnov, Fukaya and others is a generalization of "internal" category theory. In my paper "Monoidal globular categories as a natural environment ..."(Adv.Math. 136, 39-103 (1998)) I also consider a Cat-internal version of A_{\infty}-\omega-category (so it involves a weak form of interchange law)that I call monoidal globular category. A surprising coherence theorem sais that a general monoidal globular category is equivalent to a strict one (the internal category structure on objects aloows to strictify interchange low). In another my paper "Homotopy coherent category theory and A_{\infty}-structures in monoidal categories" (JPAA 123(1998),67-103) I defined an enriched version of A_{\infty}-category. So we have a honnest set of objects but morphisms are objects of a monoidal simplicial categories with a Quillen model structure. I also can define what A_{\infty} functor is and prove an appropriate coherence and homotopy invariance theorems. Another nice theorem sais that A_{\infty}-categories and their A_{-infty}-functors form an A_{infty}-category in a natural way. The simpliocial point of view on A_{\infty}-categories goes back to Boardman and Vogt book. The corresponding notion is a simplicial set satisfying some weak Kan conditions. This approach was extensively used by T.Porter and J.-M.Cordier (see T.Porter's answer on Jim's query). James Stasheff:
Since in a category we are concerned with $n$-tuples of morphisms only when they are composable, it is appropriate to similarly relax the composition operations for in defining an operad. the result is known as a partial operad and appears in two different contexts: in the mathematical physics of vertex operator algebras (VOAs) \cite{yizhi} and
Mivhael Batanin: In my work "Globular monoidal categories ..." I introduced the n-dimensional operads over trees. A 1-dimensional operad in this sense is not exatly the same as usual non-symmetric operad as every operation may have source and target and we can multiply just composable chains of operations. A one object version of this may be identify with a usual nonsymmetric operad. (In my paper I use \omega-operads). I wonder if a partial operad is the same as my 1-operad? Michael.
participants (5)
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grandis@dima.unige.it -
James Stasheff -
john baez -
Michael Batanin -
street@mpce.mq.edu.au