Under the World Tree

Homotopy Coherence and Higher Semiadditivity

Speaker: Lior Yanovski

Goal

A setting where we can do homotopy theory with monoids within a category.

  • Topological monoids (common approach to \infty-category of objects) are too rigid
  • Monoids in the homotopy category of Top\mathsf{Top} are too loose.

A middle ground is the category of homotopy coherent monoids, tensor categories with commuting Stasheff pentagons and higher diagrams:

The Stasheff associativity pentagon, a low-order coherence diagram.

Framing associativity as a coherence problem

For a homotopy theorist, associativity of multiplication for a monoid MM is connected to existence of extensions fitting in a diagram

Monoid coherence 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

Extension problems picture
,

and we define a homotopy coherent monoid to be a monoid equipped with solutions to these extension problems for all nn.

Inverses: Let M×MsM×MM \times M \xrightarrow{s} M \times M be the shear map (x,y)(x,xy)(x,y) \mapsto (x, xy). Then MM is a group if and only if ss is a bijection.

Definition: A homotopy coherent (hc) group is a hc monoid such that ss is a homotopy equivalence.

Example: For YY a topological space, X=ΩY=Map(S1,Y)X = \Omega Y = \text{Map}_{*}(\mathbb{S}^1, Y) (the basepoint-preserving maps for fixed basepoint of YY) 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 X=X0X = X_0 is isomorphic to Ω2X2\Omega^2 X_2 for some other space X2X_2, π2(X)=π0(X2)\pi_{2}(X) = \pi_{0}(X_{2}) is abelian. Since fundamental groups may be interpreted as maps from Sn\mathbb{S}^n into XX, we see that if there are spaces XmX_m such that X=ΩmXmX = \Omega^m X_m, the homotopy groups πm(X)\pi_m(X) will be abelian for m2m \geq 2. Combining with the above theorem, this should imply that homotopy coherent commutative groups correspond to infinite loopspaces. Examples:

  • Let (C,,1)(\mathscr{C}, \otimes, \mathbb{1}) be a symmetric monoidal category. Then we usually assume
X(YZ)(XY)ZX\otimes (Y \otimes Z) \simeq (X \otimes Y) \otimes Z

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
    The adjunction between the fundamental groupoid and geometric realisation functors
    taking the fundamental groupoid in one direction and the geometric realisation in the other. For example, the geometric realisation of the classifying groupoid BG\mathbb{B}G (category with one object and GG as its group of automorphisms) is the classifying space BG=BG|\mathbb{B}G| = BG. Applying the geometric realisation construction to the category Fin\mathsf{Fin}^{\simeq} of finite sets up to isomorphism (objects: one for each natural number nn, no morphisms between different sets and Hom(n,n)=Σn\text{Hom}(n,n) = \Sigma_{n} the symmetric group on nn elements) gives
Fin=nNBΣn=:M,|\mathsf{Fin}^{\simeq}| = \coprod_{n \in \mathbb{N}} B\Sigma_{n} =: \mathbb{M},

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 π0\pi_{0} gives the monoid (N,+)(\mathbb{N}, +), which we can group-complete to get (Z,+)(\mathbb{Z}, +). The corresponding 'group completion' object of M\mathbb{M} turns out to be the sphere spectrum

S=lim(S0ΩS1Ω2S2),\mathbb{S} = \varinjlim (\mathbb{S}^0 \to \Omega \mathbb{S}^1 \to \Omega^2 \mathbb{S}^2 \to \dots),

in the sense that we have a diagram

Universal monoid sphere spectrum 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

πn(S)=limkπn(Ωk(Sk))=limkπn+k(Sk)\pi_{n}(\mathbb{S}) = \varinjlim_{k} \pi_{n}(\Omega^k(\mathbb{S}^k)) = \varinjlim_{k} \pi_{n+k}(\mathbb{S}^k)

stabilises, so that if we draw a similar diagram at πn\pi_{n} 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 (C,,1)(\mathscr{C}, \otimes, \mathbb{1}), the category π0(C)\pi_{0}(\mathscr{C}) of isomorphism classes of objects in C\mathscr{C} is a commutative semiring under operations

[X]+[Y]=[XY][X][Y]=[XY],\begin{aligned} \,[X] + [Y] &= [X\cup Y] \\ [X][Y] &= [X \otimes Y], \end{aligned}

with group completion K0(C)K_{0}(\mathscr{C}) a commutative ring. We have a symmetric power operation

Sn[X]=[Xn/Σn] (coinvariants)S^n[X] = [X^{\otimes n}/\Sigma_{n}] \ (\text{coinvariants})

using the action of Σn\Sigma_{n} on XnX^{\otimes n}, and often we can also form the alternating power operation n[X]=[Xn/sgn(Σn)]\bigwedge\nolimits^{n}[X] = [X^{\otimes n}/ \text{sgn}(\Sigma_{n})] (when we have a sign representation). If C\mathscr{C} is C\mathbb{C}-linear, we also get a λ\lambda-ring structure on K0(C)K_{0}(\mathscr{C}).

Examples
  • Let C=VectCBG\mathscr{C} = \mathsf{Vect}_{\mathbb{C}}^{BG} be the category of complex vector bundles with structure group GG over a point. Then K0(C)=Rep(G)K_0(\mathscr{C}) = \mathsf{Rep}(G) inherits a λ\lambda-ring structure, from the alternating power operation.
  • Let C=FinCBG\mathscr{C} = \mathsf{Fin}^{BG}_{\mathbb{C}} be the category of all finite sets admitting GG-actions. Then K0(C)=Burn(G)K_{0}(\mathscr{C}) = \mathsf{Burn}(G) is a ring, called the Burnside ring of GG, with addition given by disjoint union of sets and multiplication by Cartesian product.

Remark: The group completion of (nNBGLn(C),)\left( \coprod_{n \in \mathbb{N}} B\mathrm{GL}_{n}(\mathbb{C}), \oplus \right) in the category of spectra is an object usually denoted by kuku, the spectrum of topological complex K-theory. The name comes from the fact that for a compact object XX in the category, K0(X)=[X,ku],K_{0}(X) = [X, ku], the maps from XX to kuku. With the tensor product \otimes of complex vector space, kuku comes equipped with hc commutative ring structure.

Example - Power Elements Let RR be any commutative ring spectrum (in the topological sense, so we have an infinite suspension diagram of rings). Then an element xRx \in R can be thought of as an arrow in a diagram of hc objects

Diagram of power operations
.

Since M=nNBΣn\mathbb{M} = \coprod_{n \in \mathbb{N}} B\Sigma_{n} we have maps from the point to each one-point space BΣnB\Sigma_{n}. Now a map BΣnRB\Sigma_{n} \to R picks out an element xnRBΣnx^n \in R^{B\Sigma_{n}} the hc ring of all objects with automorphism group Σn\Sigma_{n} (identified with Map(BΣn,R)\mathsf{Map}(B\Sigma_{n}, R)), and we have π0(RBΣn)=R0(BΣn),\pi_{0}(R^{B\Sigma_{n}}) = R^0(B\Sigma_{n}), where R0=π0(R)R^0 = \pi_{0}(R) (so the RHS is the ordinary points of the ordinary ring RR which have Σn\Sigma_{n}-automorphisms). Coherence is equivalent to the statement that the diagram

Coherence for power operationscommutes,

where the object on the bottom is the quotient groupoid (every object of RnR^n has Σn\Sigma_{n}-automorphisms). Now since we have an arrow α:R0(M)R0\alpha: R^0(\mathbb{M}) \to R^0 as above, we get power elements α(xm)R\alpha(x^m) \in R for all mm 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 MOMO such that πn(MO)\pi_{n}(MO) is the category of stably framed smooth nn-manifolds up to cobordism, and [X,MO][X, MO] gives cobordism cohomology for a topological space XX.
  • The Morava E-theories form a sequence of commutative ring spectra, with
    • E0CE_0 \approx \mathbb{C}
    • E1kup^E_1 \approx k\hat{u_{p}} and higher EE'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 xΩ2S2x \in \Omega^2 \mathbb{S}^2 we have arrows

1xx1 σx,x1x1x11 \sim x\cdot x^{-1} \overset{ \ \sigma_{x,x^{-1}}}\sim x^{-1}\cdot x \sim 1

(using a Σ2\Sigma_{2}-action on the product xx1x\cdot x^{-1}); the loop corresponds to the Hopf map S1Ω2S2\mathbb{S}^1 \to \Omega^2 \mathbb{S}^2, ie S3ηS2\mathbb{S}^3 \xrightarrow{\eta} \mathbb{S}^2.

Orbits: If we have a categorical group action BGZCBG \xrightarrow{Z} \mathscr{C} factoring through the one-point space BGptCBG \to \text{pt} \to \mathscr{C}, then we have limZ=Z//G\varinjlim Z = Z//G, identifying ZZ with its one-object image. In particular, the limit over [n]{Xi}i[n]C[n] \xrightarrow{\{X_{i}\}_{i \in [n]}} \mathscr{C} is given by lim[n]Xi=X1Xn\varinjlim_{[n]}X_{i} = X_{1} \cup \dots \cup X_{n}.

Semiadditivity

Definition: A space XX is n-finite if πk(X,x)=0\pi_{k}(X, x) = 0 for all k>nk > n and if all homotopy groups πk(X,x)\pi_k(X, x) are finite, for every xXx \in X and kN.k \in \mathbb{N}.

  • 0-finite spaces are the finite discrete spaces, up to homotopy equivalence.
  • 1-finite spaces are unions of classifying spaces BGi\mathbb{B}G_{i}, where each GiG_i is a finite group.

Definition: An n-commutative monoid is a (Segal) space XX such that:

  • For every nn-finite space A\mathcal{A}, the left Kan extension A:XAX\int_{\mathcal{A}}: X^\mathcal{A} \to X 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
Diagram of Kan extension and invariants functor giving a categorical 'induced representation'.

Example: If X=QX = \mathbb{Q} (more generally, any divisible commutative monoid) and we have a constant map BGfQBG \xrightarrow{f} \mathbb{Q}, the left Kan extension is BGf=1Gf(x)\int_{BG}f = \frac{1}{|G|}f(x). So we see that the extension is providing a generalisation of 'averaging over GG'.

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 X1,,XnX_1, \dots, X_{n} of objects,

X1XnX1××XnX_{1} \cup \dots \cup X_{n} \cong X_{1} \times \dots \times X_{n}

via the canonical morphism X1XnX1××XnX_{1} \cup \dots \cup X_{n} \to X_{1} \times \dots \times X_{n}.

Definition (Hopkins-Lurie): An \infty-category C\mathscr{C} is n-semiadditive if for every diagram X:ACX: A \to \mathscr{C} with AA an n-finite space, there is a canonical isomorphism

limA XlimA X.\varinjlim_{A} \ X \cong \varprojlim_{A} \ X.

If X,YCX, Y \in \mathscr{C} are 00-semiadditive, f,g:XYf, \, g : X \to Y we can construct the diagram

Homotopy-coherent addition
recovering and generalising addition to the homotopy-coherent setting!

Theorem: If C\mathscr{C} is nn-semiadditive for all X,YCX, Y \in \mathscr{C}, MapC(X,Y)\text{Map}_{\mathscr{C}}(X,Y) has a canonical nn-commutative monoid structure.

  • In the category Sp(p)\mathsf{Sp}_{(p)} of pp-localised spectra, there is a sequence of ringed spectra K(n)K(n) for 0n0 \leq n \leq \infty, called the Morava K-theories. We have K(0)=H(Q)K(0) = H(\mathbb{Q}) the spectrum of rational cohomology, and K()=HFpK(\infty) = H\mathbb{F}_{p} the spectrum of mod pp cohomology.
  • If one knows K(n)K(n)-locality and support theorems, then one can show that SpK(n)Sp(p)\mathsf{Sp}_{K(n)} \xhookrightarrow{} \mathsf{Sp}_{(p)}.

Theorem(Hopkins-Lurie): The categories SpK(n)\mathsf{Sp}_{K(n)} are \infty-semiadditive, for n<n < \infty.

Theorem(Y.): The categories SpT(n)\mathsf{Sp}_{T(n)} for n<n < \infty are also \infty-semiadditive.

  • If RR is a K(n)K(n)-(or T(n)T(n)-)local commutative ring spectrum, all maps RBΣnRR^{B\Sigma_{n}} \to R are of the form xBΣnaxnx\mapsto \int_{B\Sigma_{n}}ax^n, for aRBΣna \in R^{B\Sigma_{n}}.

Example: In height 00 and over Q\mathbb{Q}, all possible power operations are given by

a0+a1x+a22!x2++ann!xn.a_{0} + a_{1}x + \frac{a_{2}}{2!}x^2 + \dots + \frac{a_{n}}{n!}x^n.