This post is an exposition of the material in the paper “Homotopy is not concrete” by P. Freyd, of whose existence I learned from this MO discussion.

A category {\mathcal{C}} is concrete if there is a faithful functor {F: \mathcal{C} \rightarrow \mathbf{Sets}}. Most of the categories one initially encounters are in fact concrete: categories of groups, rings, modules, Lie algebras, and so on, and one can think of them as consisting of “structured sets” and “morphisms respecting that structure.” Every small category is concrete, because one can take the Yoneda embedding

\displaystyle \mathcal{C} \rightarrow \mathbf{Sets}^{\mathcal{C}^{op}}

followed by the product functor {\mathbf{Sets}^{\mathcal{C}^{op}}\rightarrow \mathbf{Sets}}.

Nonetheless, not every category is concrete, and the following example shows that a very natural one is not:

 

Theorem 1 (Freyd) The homotopy category {\mathcal{H}ot_*} of pointed spaces is not concrete.

 

In other words, a homotopy type is somehow too complex to be encoded simply as a set with appropriate structure.

The idea of the proof is essentially the following. In a category of structured sets, a given object can only have so many subobjects, because a set has only so many subsets. But there are categories where an object may have an enormous collection of subobjects, because the definition of a subobject is purely arrow-theoretic. So a category where objects can have lots of subobjects is probably not concrete. (more…)

I’m not an expert on tech policy (or policy in general), but as far as I can tell the proposed “Stop Online Piracy Act” is really atrocious in its (possibly unconstitutional?) over-reach, and would probably be very bad for bloggers, mathematics, and the internet. Following Tim Gowers, Wikipedia, and others, I’ll be blocking this blog tomorrow. I couldn’t find out a good way to do this (those with a custom stylesheet can directly edit things to do so), so like Gowers, I’ll make this blog private for a day.

Edit: It actually seems that WordPress has provided a means to do this directly. Let’s see how that works.

[Apologies in the delay in posts on the Segal paper -- there are a couple of things I'm confused on that are preventing me from proceeding.]

A classical problem (posed by Serre) was to determine whether there were any nontrivial algebraic vector bundles over affine space {\mathbb{A}^n_k}, for {k} an algebraically closed field. In other words, it was to determine whether a finitely generated projective module over the ring {k[x_1, \dots, x_n]} is necessarily free. The topological analog, whether (topological) vector bundles on {\mathbb{C}^n} are trivial is easy because {\mathbb{C}^n} is contractible. The algebraic case is harder.

The problem was solved affirmatively by Quillen and Suslin. In this post, I would like to describe an elementary proof, due to Vaserstein, of the Quillen-Suslin theorem. (more…)

(This is the second post devoted to unpacking some of the ideas in Segal’s paper “Categories and cohomology theories.” The first is here.)

Earlier, I described an observation (due to Beck) that loop spaces could be characterized as algebras over the monad {\Omega \Sigma}. At least, any loop space was necessarily an algebra over that monad, and conversely any algebra over that monad was homotopy equivalent to a loop space. There is an alternative and compelling idea of Segal which gives a condition somewhat easier to check.

As far as I understand, most of the different approaches to delooping a space consist of imitating the classical construction for a topological group {G}: the construction of the space {BG}. It is known that any topological group {G} is (weakly) homotopy equivalent {\Omega BG}, and conversely (though perhaps it is not as well known) that any loop space is homotopy equivalent to a topological group. (This can be proved using the simplicial construction of Kan.) Given a space (which may not be a topological group), the idea is that delooping machinery will assume given just enough structure to build something analogous to the classifying space, and then build that. This is, for instance, how the construction of Beck ran.

Here’s Segal’s idea; it is quite similar to the {\Gamma}-idea. Given a topological group {G}, we can construct {BG} using a standard simplicial construction. If {G} is only a group object in the homotopy category, we can’t run this construction. Segal decides just to assume that one has given the data of a simplicial object that behaves like {BG } should and runs with that.

The starting point is that one can encode the structure of a monoid in a simplicial set. Given a monoid {G}, the simplicial set {BG} has the following properties.

  1. {(BG)_0} is a point.
  2. The map {(BG)_n \rightarrow \prod_{i=1}^n (BG)_1} induced by the {n} inclusions {[1] \rightarrow [n]} (sending {0} and {1} to consecutive elements) is an isomorphism.

In fact, if we have any simplicial set with the above properties, it determines a unique monoid. This is proved in a similar way. If {X_\bullet} is such a simplicial set, then we take {X_1} as the underlying set of the monoid, and the map {X_1 \times X_1 \rightarrow X} comes from the boundary map {X_2 \rightarrow X_1}; the identity element comes from the map {X_0 = \ast \rightarrow X_1}. So monoids can be described as simplicial sets satisfying certain properties (just as commutative monoids can).

As before, we can weaken this by replacing “isomorphism” by “homotopy equivalence.” (more…)

commutative monoid is a set {A} together with a multiplication map {m: A \times A \rightarrow A} and a distinguished unit element {e \in A}, satisfying certain identities. Let us say that we are interested in a homotopical version of this idea, especially a version of the idea of an abelian group. Then, we could try to work in the category of topological abelian groups, but this is somewhat uninteresting from the point of view of homotopy theory: every topological abelian is weakly homotopy equivalent to a product of Eilenberg-MacLane spaces. Alternatively, we could demand that one has a topological space together with a multiplication law which is commutative up to homotopy; however, as we’ve seen, this isn’t enough structure to perform a construction such as the classifying space.

Segal’s idea, in his paper “Categories and cohomology theories,” is to rephrase the definition of a commutative monoid in such a way as to require only a bunch of sets and maps with them, such that certain ones are isomorphisms. This will lead to an immediate homotopical generalization: replace “isomorphism” with “weak equivalence.”

1. Segal’s category of finite sets

We can define the category (due to Segal) {\mathcal{F}in_*} of finite sets and partially defined maps as follows. The objects of {\mathcal{F}in_*} are finite sets. A morphism {A \rightarrow B} in {\mathcal{F}in_*} is the data of a subset {A' \subset A} and a map {A' \rightarrow B}. The composition of two partially defined maps is just the ordinary composition, defined wherever it makes sense.

Suppose {A} is a commutative monoid. We can package the data of {A} into a functor

\displaystyle \widetilde{A}: \mathcal{F}in_* \rightarrow \mathrm{Set}

by sending a finite set {S} to {A^S}. Given a partially defined map {\theta} between {S} and {S'}, we get a map {A^S \rightarrow A^{S'}} sending a tuple {(x_s)} to the following tuple:

\displaystyle \theta(x)_{s'} = \sum_{s \in \theta^{-1}(s)} x_s.

Thus, to each commutative monoid, we can associate a functor {\widetilde{A}: \mathcal{F}in_* \rightarrow \mathrm{Set}}. The functors {\widetilde{A}} have the following properties:

  1. {\widetilde{A} (\emptyset) = \ast}.
  2. For each {n}, {\widetilde{A}(n) \rightarrow \prod_{i=1}^n \widetilde{A}(1)} is an isomorphism, where the maps are induced by the maps {\langle n\rangle \rightarrow \langle 1\rangle} defined only on {i}.

In fact, these two properties are enough to recover {A} and its abelian group structure. Let us be a bit more systematic. We let {\theta_i: \langle n\rangle \rightarrow \langle 1\rangle} be the maps listed above; they are very simple, being defined only at one point (that is, {i}). Let us suppose we have a functor {F: \mathcal{F}in_* \rightarrow \mathrm{Set}} such that {F(\emptyset) = \ast} and such that for each {n}, the product map

\displaystyle F(\langle n\rangle) \stackrel{\prod \theta_i}{\rightarrow} \prod_i F(\langle 1\rangle)

is an isomorphism. Then there is a canonically determined abelian monoid structure on {F(\langle 1\rangle)}, and one can phrase this as an equivalence of categories between such functors and abelian monoids. (more…)

The present post is motivated by the following problem:

Problem: Given a pointed space {X}, when is {X} of the homotopy type of a {k}-fold loop space {\Omega^k Y} for some {Y}?

One of the basic observations that one can make about a loop space {\Omega Y} is that admits a homotopy associative multiplication map

\displaystyle m: \Omega Y \times \Omega Y \rightarrow \Omega Y.

Having such an H structure imposes strong restrictions on the homotopy type of {\Omega Y}; for instance, it implies that the cohomology ring {H^*(\Omega Y; k)} with coefficients in a field is a graded Hopf algebra. There are strong structure theorems for Hopf algebras, though. For instance, in the finite-dimensional case and in characteristic zero, they are tensor products of exterior algebras, by a theorem of Milnor and Moore. Moreover, for a double loop space {\Omega^2 Y}, the H space structure is homotopy commutative.

Nonetheless, it is not true that any homotopy associative H space has the homotopy type of a loop space. The problem with mere homotopy associativity is that it asserts that two maps are homotopic; one should instead require that the homotopies be part of the data, and that they satisfy coherence conditions. The machinery of operads was developed to codify these coherence conditions efficiently, and today it seems that one of the powers of higher (at least, {(\infty, 1)}) category theory is the ability to do this in a much more general context.

For this post, I want to try to ignore all this operadic and higher categorical business and explain the essential idea of the delooping construction in May’s “The Geometry of Iterated Loop Spaces”; this relies on some category theory and a little homotopy theory, but the explicit operads play very little role. (more…)

Let {f: S^{2n-1} \rightarrow S^n} be a map with {n >1}. Associated to this, one can form a CW complex {M_f = D^{2n} \cup_f S^n}; that is, we attach a {2n}-cell to {S^n} via the map {f}. This CW complex has one cell in dimension {n} and one cell in dimension {2n} (and one cell in dimension {0}). The map {D^{2n} \rightarrow M_f} determines a generator {\iota_{2n}} of {H^{2n}(M_f; \mathbb{Z})} and the map {S^n \rightarrow M_f} determines a generator {\iota_n} of {H^{n}(M_f; \mathbb{Z})}; there are no other elements in cohomology other than the unit. Consequently, we have

\displaystyle \iota_n^2 = a \iota_{2n} , \quad a \in \mathbb{Z}.

Definition 1 The number {a} as above such that {\iota_n^2 = a \iota_{2n}} is the Hopf invariant of {f}.

The homotopy type of {M_f} determines only on the homotopy class of {f}, so the Hopf invariant is a homotopy invariant.

Example 1 The Hopf fibration {f: S^3 \rightarrow S^2} is, by definition, the map such that the mapping cone {M_f} is {\mathbb{CP}^2}; it follows that the Hopf fibration has Hopf invariant one.

The Hopf invariant is clearly identically zero for {n} odd, but when {n} is even the Hopf invariant is never identically zero; in fact, it defines a homomorphism

\displaystyle \pi_{2n-1}(S^n) \rightarrow \mathbb{Z},

which for {n} even has image containing the even integers. (This is where the exceptional {\mathbb{Z}} summand in the homotopy groups of spheres comes from.)

A classical problem in topology was the following:

Question: For which {n} does there exist a map of Hopf invariant one? (more…)

Cathy O’Neill’s new blog Mathbabe seems to be fairly active already, but I thought I would promote it here in case some of this blog’s readers have not seen it.  I don’t think I would be able to summarize this extremely interesting and varied blog about quantitative issues, politics, and mathematics, so you should read it instead of listening to me recommend it!

Let {M} be a compact manifold, {E, F} vector bundles over {M}. Last time, I sketched the definition of what it means for a differential operator

\displaystyle D: \Gamma(E) \rightarrow \Gamma(F)

to be elliptic: the associated symbol

\displaystyle \sigma(D): \pi^* E \rightarrow \pi^* F, \quad \pi: T^* X \rightarrow X

was required to be an isomorphism outside the zero section. The goal of the index theorem is to use this symbol {\sigma(D)} to compute the index of {D}, which we saw last time was a well-defined number

\displaystyle \mathrm{index} D = \dim \ker D - \dim \mathrm{coker} D \in \mathbb{Z}

invariant under continuous perturbations of {D} through elliptic operators (by general facts about Fredholm operators).

The main observation is that {D}, in virtue of its symbol, determines an element of {K(TX)}. (Henceforth, we shall identify the tangent bundle {TX} with the cotangent bundle {T^*X}, by choice of a Riemannian metric; the specific metric is not really important since {K}-theory is a homotopy invariant.) In fact, we have that {K(TX)} is the (reduced) {K}-theory of the Thom space, so it is equivalently {K(BX, SX)} for {BX} the unit ball bundle and {SX} the unit sphere bundle. But we have seen that to give an element of {K(BX, SX)} is the same as giving a pair of vector bundles on {BX} together with an isomorphism on {SX}, modulo certain relations.

Observation: The symbol of an elliptic operator determines an element in {K(TX)}. (more…)

Today I would like to blog about a result of Atiyah from the 1950s, from his paper “Bott periodicity and the parallelizability of the spheres.” Namely:

Theorem 1 (Atiyah) On a nine-fold suspension {Y = \Sigma^9 X} of a finite complex, the Stiefel-Whitney classes of any real vector bundle vanish.

In particular, this means that any real vector bundle on a sphere S^n, n \geq 9 cannot be distinguished using Stiefel-Whitney classes from the trivial bundle. The argument relies on the Bott periodicity theorem and some calculations with Stiefel-Whitney classes. There is also an analog for the Chern classes of complex vector bundles on spheres; they don’t necessarily vanish but are highly divisible.

These sorts of integrality theorems often have surprising geometric consequences. In this post, I’ll discuss the classical problem of when spheres admit almost-complex structures, a problem one can solve using the second of the integrality theorems mentioned above. Atiyah was originally motivated by the question of parallelizability of the spheres. (more…)

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