Speaker: Lior Yanovski
Goal
A setting where we can do homotopy theory with monoids within a category.
- Topological monoids (common approach to -category of objects) are too rigid
- Monoids in the homotopy category of are too loose.
A middle ground is the category of homotopy coherent monoids, tensor categories with commuting Stasheff pentagons and higher diagrams:

Framing associativity as a coherence problem
For a homotopy theorist, associativity of multiplication for a monoid is connected to existence of extensions fitting in a diagram

(using the appropriate sphere/disk objects in the category, eg coming from initial/terminal objects and categorical constructions). More generally, we have a family of extension problems

and we define a homotopy coherent monoid to be a monoid equipped with solutions to these extension problems for all .
Inverses: Let be the shear map . Then is a group if and only if is a bijection.
Definition: A homotopy coherent (hc) group is a hc monoid such that is a homotopy equivalence.
Example: For a topological space, (the basepoint-preserving maps for fixed basepoint of ) is a hc group.
(rough statement of) Theorem: Homotopy coherent groups correspond bijectively to loop spaces.
Recall that the Eckmann-Hilton argument says that if a space is isomorphic to for some other space , is abelian. Since fundamental groups may be interpreted as maps from into , we see that if there are spaces such that , the homotopy groups will be abelian for . Combining with the above theorem, this should imply that homotopy coherent commutative groups correspond to infinite loopspaces. Examples:
- Let be a symmetric monoidal category. Then we usually assume
up to isomorphism, together with higher coherence of the isomorphisms (Stasheff pentagon is used as an associator and implies higher diagrams). These coherences can be thought as belonging to the subcategory consisting of objects and invertible morphisms (so there is a groupoid perspective on this).
- Recall that we have functors taking the fundamental groupoid in one direction and the geometric realisation in the other. For example, the geometric realisation of the classifying groupoid (category with one object and as its group of automorphisms) is the classifying space . Applying the geometric realisation construction to the category of finite sets up to isomorphism (objects: one for each natural number , no morphisms between different sets and the symmetric group on elements) gives

which has a homotopy coherent commutative monoid structure given by disjoint union. The resulting monoid is the free monoid on one element (note: the monoid itself is not commutative but its higher associations are). Applying gives the monoid , which we can group-complete to get . The corresponding 'group completion' object of turns out to be the sphere spectrum
in the sense that we have a diagram

Of course, for this to be the right choice of completion we need more than just the same underlying monoid as the group completion, but I didn't catch this detail in the talk. For one hint in this direction, recall that by the Freudenthal suspension theorem, the sequence
stabilises, so that if we draw a similar diagram at we are getting the stable stems of the sphere spectrum along the bottom.
Decategorification
One use for homotopy coherent constructions is decategorification, reducing the full collection of hc data to structure which is easier to carry around.
For a symmetric monoidal category , the category of isomorphism classes of objects in is a commutative semiring under operations
with group completion a commutative ring. We have a symmetric power operation
using the action of on , and often we can also form the alternating power operation (when we have a sign representation). If is -linear, we also get a -ring structure on .
Examples- Let be the category of complex vector bundles with structure group over a point. Then inherits a -ring structure, from the alternating power operation.
- Let be the category of all finite sets admitting -actions. Then is a ring, called the Burnside ring of , with addition given by disjoint union of sets and multiplication by Cartesian product.
Remark: The group completion of in the category of spectra is an object usually denoted by , the spectrum of topological complex K-theory. The name comes from the fact that for a compact object in the category, the maps from to . With the tensor product of complex vector space, comes equipped with hc commutative ring structure.
Example - Power Elements Let be any commutative ring spectrum (in the topological sense, so we have an infinite suspension diagram of rings). Then an element can be thought of as an arrow in a diagram of hc objects

Since we have maps from the point to each one-point space . Now a map picks out an element the hc ring of all objects with automorphism group (identified with ), and we have where (so the RHS is the ordinary points of the ordinary ring which have -automorphisms). Coherence is equivalent to the statement that the diagram
commutes,where the object on the bottom is the quotient groupoid (every object of has -automorphisms). Now since we have an arrow as above, we get power elements for all from our original diagram. (This is probably only partially correct, I am missing definitions and details to make this precise) I think we want this to explain the power elements/formal group laws of Lubin, Lurie et al
- There is a Thom spectrum such that is the category of stably framed smooth -manifolds up to cobordism, and gives cobordism cohomology for a topological space .
- The Morava E-theories form a sequence of commutative ring spectra, with
- and higher 's being related to things like Witt vector cohomology. I think these are used in topology to study torsion phenomena.
Example: The Hopf fibration can be constructed by decategorification. In the sphere spectrum, taking we have arrows
(using a -action on the product ); the loop corresponds to the Hopf map , ie .
Orbits: If we have a categorical group action factoring through the one-point space , then we have , identifying with its one-object image. In particular, the limit over is given by .
Semiadditivity
Definition: A space is n-finite if for all and if all homotopy groups are finite, for every and
- 0-finite spaces are the finite discrete spaces, up to homotopy equivalence.
- 1-finite spaces are unions of classifying spaces , where each is a finite group.
Definition: An n-commutative monoid is a (Segal) space such that:
- For every -finite space , the left Kan extension exists
- There is homotopy-coherent associativity and a homotopy-coherent unit
- Analogous to taking the orbits of the induced representation, we have a commuting diagram

Example: If (more generally, any divisible commutative monoid) and we have a constant map , the left Kan extension is . So we see that the extension is providing a generalisation of 'averaging over '.
Definition: A category is (-1)-semiadditive or pointed if its intial and terminal object are isomorphic.
Definition: A category is (0-)semiadditive if for all finite collections of objects,
via the canonical morphism .
Definition (Hopkins-Lurie): An -category is n-semiadditive if for every diagram with an n-finite space, there is a canonical isomorphism
If are -semiadditive, we can construct the diagram

Theorem: If is -semiadditive for all , has a canonical -commutative monoid structure.
- In the category of -localised spectra, there is a sequence of ringed spectra for , called the Morava K-theories. We have the spectrum of rational cohomology, and the spectrum of mod cohomology.
- If one knows -locality and support theorems, then one can show that .
Theorem(Hopkins-Lurie): The categories are -semiadditive, for .
Theorem(Y.): The categories for are also -semiadditive.
- If is a -(or -)local commutative ring spectrum, all maps are of the form , for .
Example: In height and over , all possible power operations are given by
