On the -equivariant dual Steenrod algebra
Abstract
We compute the -equivariant dual Steenrod algebras associated to the constant Mackey functors and , as -modules. The -spectrum is not a direct sum of -graded suspensions of when is odd, in contrast with the classical and -equivariant dual Steenrod algebras.
Introduction
For over a decade, since the Hill-Hopkins-Ravenel solution of the Kervaire invariant one problem [HHR16], there has been great success in using exotic homotopy theories, like -equivariant homotopy theory and motivic homotopy theory, to study classical homotopy theory at the prime 2. A key foundational input to many of these applications is the computation of the appropriate version of the dual Steenrod algebra, , which was carried out by Hu-Kriz [HK01] in -equivariant homotopy theory and by Voevodsky [Voe03] in motivic homotopy theory. One of the major obstacles to carrying out a similar program at odd primes is that we do not understand the structure of the dual Steenrod algebra in -equivariant homotopy theory. The purpose of this paper is to make some progress towards this goal.
To motivate the statement of our main result, recall that
we have the following description of the
classical, -local dual Steenrod algebra
as a -algebra111We learned this fact from John Rognes.
One proof is to base change the equivalence
to and use that the Hurewicz image
of the βs are , mod decomposables.
Here the tensor product is taken over the sphere spectrum, denotes the free -algebra on a class , and the classes live in degree . Modding out by causes each of the above cofibers to split into two classes related by a Bockstein; modding out by once more introduces the class and recovers Milnorβs computation of , as an -algebra.
In the -equivariant case our description involves a similar decomposition but is more complicated in two ways:
-
β’
Rather than extending the class to a map from using the multiplication on , we will want to choose as generators a mixture of ordinary powers of and of norms, , of .
-
β’
Rather than modding out by the relation ββ we will need to enforce the relation that ββ, where is an equivariant lift of to an element in nontrivial -degree. We will then also need to enforce the relation .
To make this precise, we will assume that the reader is comfortable with equivariant stable homotopy theory as used, for example, in [HHR16], and introduce the following conventions, in force throughout the paper:
-
β’
We will use to denote the regular representation of .
-
β’
We will use to denote the representation of on where the generator acts by .
-
β’
We denote by the map of -spectra arising from the degree cover . Weβll denote the cofiber of by . Note that the underlying nonequivariant spectrum of is the Moore space .
-
β’
If is a spectrum, we will denote by the Hill-Hopkins-Ravenel norm of , which is a -equivariant refinement of the ordinary spectrum .
-
β’
We denote by and the -equivariant Eilenberg-MacLane spectra associated to the constant Mackey functors at and , respectively.
-
β’
We use to denote the symmetric monoidal structure on genuine -spectra, (often denoted by , the smash product).
-
β’
The degree map
is a -local equivalence when , so, when working -locally, we will often make this identification implicitly. For example, we may write
-
β’
We use to denote the -graded homotopy groups of a spectrum, so that, when is a virtual representation, .
Now we can give a somewhat ad-hoc description of the equivariant refinements of the building blocks in .
Construction.
Let be a formal variable in an -grading . Define a -spectrum as follows:
where is the mod Moore spectrum. We denote the inclusion of the summand by
the restriction of to the bottom cell by , and the inclusion of the final summand by . We denote by
the restriction of to the bottom cell of the mod Moore spectrum.
Now suppose that is a -ring spectrum equipped with a norm . If we have a class such that , it follows that (see the proof of Lemma 4.4), so we may produce a map
which only depends on the choice of the nullhomotopy witnessing .
We can now state our main theorem.
Theorem A.
There are equivariant refinements
of the nonequivariant classes which satisfy the relation . For any choice of witness for these relations, the resulting map
is an equivalence.
As an immediate corollary we have:
Corollary.
With notation as above, we have
where is dual to the Bockstein, in degree and . In particular, since is indecomposable at odd primes, the spectrum is not a direct sum of -graded suspensions of at odd primes.
Remark.
When we have an accidental splitting , where is the sign representation.
Remark.
One can show that splits as . It follows that splits as a direct sum of cell complexes with at most 2 cells.
Our result raises a few natural questions which would be interesting to investigate.
Question 1.
When specialized to , how does our basis compare to the Hu-Kriz basis?
Question 2.
The geometric fixed points of are given by , where is the conjugate of , a class in degree . It is possible to understand what happens to the generators and upon taking geometric fixed points. One is left with trying to understand the remaining class hit by on geometric fixed points. We donβt know what this should be. One guess that seems consistent with computations is that this class is given, up to conjugating the and modding out by , by:
It would be useful for computations to sort out what actually occurs.
Question 3.
Is it possible to profitably study the -based Adams spectral sequence using this decomposition? Since is not flat over , one would be forced to start with the -term. But this is not an unprecedented situation (e.g. Mahowald had great success with the -based Adams spectral sequence).
Question 4.
Can one describe the multiplication on in terms of our decomposition?
Relation to other work
As we mentioned before, we were very much motivated by the description of the -equivariant dual Steenrod algebra given by Hu-Kriz [HK01]. That said, our generators are slightly different than the Hu-Kriz generators when we specialize to . For example, the generator lives in degree , whereas the Hu-Kriz generator lives in degree .222In this low degree, it seems likely that, modulo decomposables, we have and that is recovered from by restricting along . Hill and Hopkins have also obtained a presentation of the -dual Steenrod algebra, using quotients of and its norms, which is similar in style to the one obtained here.
At odd primes, Caruso [Car99] studied the -equivariant Steenrod algebra, , essentially by comparing with the Borel equivariant Steenrod algebra and the geometric fixed point Steenrod algebra, and was able to compute the ranks of the integer-graded stems. There is also work of OruΓ§ [Oru89] computing the dual Steenrod algebra for the Eilenberg-MacLane spectra associated to Mackey fields (which does not include ).
In the Borel equivariant setting, the dual Steenrod algebra is given by the action Hopf algebroid for the coaction of the classical dual Steenrod algebra on (see [Gre88]).
There is also related work from the first and second authors. The first author produced a splitting of in [San19] using the symmetric power filtration. This summands in that splitting were roughly given by the homology of classifying spaces, and were much larger than the summands produced here. The second author and Jeremy Hahn showed [HW20] that can be obtained as a Thom spectrum on . The Thom isomorphism then reduces the study of the dual Steenrod algebra to the computation of the homology of . Understanding the relationship between this picture and the one in this article is work in progress.
Acknowledgements
We thank Jeremy Hahn and Clover May for excellent discussions over the course of this project. We thank Mike Hill for generously sharing his time and his ideas, especially the idea to use the norm to build some of the generators of the dual Steenrod algebra. We apologize to those awaiting the publication of these results for the long delay.
1 Outline of the proof
To motivate our method of proof, letβs first revisit the classical story. We are interested in where the classes come from, and why they are annihilated by .
Recall that the homology of is a divided power algebra
where is dual to the first Chern class . Write . Since , we have a map of spectra
and hence a homology suspension map
which annihilates elements decomposable with respect to the product structure on . We can take333Depending on ones preferences, this might be the conjugate of the generator you want; but we are only really concerned with these classes modulo decomposables. . The relation follows from the fact that is, up to a -local unit, decomposable as in .
In the equivariant case, we will proceed similarly.
-
Step 1.
Compute the homology of and use the homology suspension to define classes in .
-
Step 2.
Use information about the product structure on the homologies of and to deduce relations for these classes, and hence produce the map described in Theorem A.
-
Step 3.
Verify that the map in Theorem A is an equivalence by proving that it is an underlying equivalence and an equivalence on geometric fixed points.
The first step is carried out in Β§2 and Β§3 by identifying with an equivariant version of and then specializing a computation due to Lewis [Lew88], which we review in our context. The second step is carried out in Β§4. The third and final step is carried out in Β§6 using a lemma proven in Β§5 that allows us to check that the map on geometric fixed points is an equivalence by just verifying that the source and target have the same dimensions in each degree.
2 Homology of
Recall that we have the -space classifying equivariant principal -bundles. The following lemmas give two useful ways of thinking about this space.
Lemma 2.1.
The complex projective space is a model for , where the generator of acts on through ring maps by . Here is the ordinary polynomial ring over , and the projective space inherits an action in the evident way.
Lemma 2.2.
The space is a model for .
Proof.
The map
to the infinite symmetric product, which sends a polynomial to its set of roots (with multiplicity), is an equivariant homeomorphism. The group-completion of the latter is a model for by the equivariant Dold-Thom theorem. But is already group-complete: the monoid of connected components of the fixed points is . β
Remark 2.3.
The reader may object that the definition of makes no reference to , so how does know about this representation rather than for some coprime to ? The answer is that, in fact, each of the Eilenberg-MacLane spaces coincide for such : we have an equivalence of -modules
whenever . This follows from the computations in [FL04, Proposition 9.2], for example.
The filtration of by the subspaces of polynomials of degree at most gives a filtration of .
Lemma 2.4.
There is a canonical equivalence
where .
Proof.
This follows from a more general observation. If is a one-dimensional complex representation, and is an arbitrary complex representation, then the function assigning a linear map to its graph,
is an equivariant homeomorphism. So it induces an equivalence on one-point compactifications
β
The next proposition now follows from [Lew88, Proposition 3.1].
Proposition 2.5 (Lewis).
The above filtration on splits after tensoring with , giving an equivalence
where
In particular, for we have .
We will also need some information about the multiplicative structure on homology.
Lemma 2.6.
Writing to mean that for some , we have
Proof.
Using the model for given by , we see that, in fact, has the structure of a filtered monoid. It follows that the product in homology respects the filtration by the classes . Thus, for , we have:
where the coefficients lie in . When we see that the virtual representations have positive virtual dimension and their fixed points also have positive virtual dimension. The homotopy of vanishes in these degrees (see, e.g., [FL04, Theorem 8.1(iv)]), so we must have
where and when . In both cases, the restriction map on is injective in this degree, so the result follows from the nonequivariant calculation. β
3 Suspending classes
We begin with some generalities. If is any -spectrum, we have the counit
which induces a map
called the homology suspension. Just as in the classical case, annihilates decomposable elements in .
Construction 3.1.
For , we define
as the homology suspension of the element . Here we use the identification
4 Two relations in homology
We begin with a brief review of norms, transfers, and restrictions.
Remark 4.1 (Transfer and restriction).
Given a nonequivariant equivalence , we define
and
For example, when and , then .
Changing the equivalence has the effect of altering these classes by ; in our case the representations in question have canonical orientations so this will not be a concern. Given a map we have a relation:
Remark 4.2 (Norms).
If a -spectrum has a map , then, given an underlying class , we may define a norm by the composite
The underlying nonequivariant class is given by .
Our goal in this section is to prove the following two lemmas.
Lemma 4.3.
The classes satisfy .
Lemma 4.4.
The classes satisfy .
In fact, the second relation follows from the first.
Proof of Lemma 4.4 assuming Lemma 4.3.
Since , the class is the transfer of the class into degree . Notice that (after identifying the suspensions with for ), and the transfer of into this degree is , so we have
β
Proof of Lemma 4.3.
By Lemma 2.6, we have so that , since annihilates decomposables. For the remaining classes, consider the commutative diagram
where . Thus, to show that for , it is enough to show that is decomposable in for .
Write
where the elements are the standard module generators of , and write . To show that is decomposable for , it is enough to establish the following two claims:
-
(a)
, and
-
(b)
.
Claim (b) is just the classical computation of the product in homology for . For claim (a), let denote the fundamental class in cohomology for and the same for . Then we have by design, and hence
The map on homology is now determined by the relation
Since is a transferred class, the value above is also a transfer, and hence determined by its restriction to an underlying class. But and we clearly have , which agrees with the restriction of . This completes the proof. β
5 Digression: Detecting equivalences nonequivariantly
The goal of this section is to establish a criterion for detecting equivalences of -modules. We recall that
where the class in degree 2 arises from taking the geometric fixed points of the Thom class .
Proposition 5.1.
Let be a map of -modules which are bounded below. Assume the following conditions are satisfied:
-
(i)
is an underlying equivalence.
-
(ii)
and are finite dimensional of the same rank, for all .
-
(iii)
and are graded-free -modules.
Then is an equivalence.
We will deduce this proposition from the following one, which relates geometric and Tate fixed points.
Proposition 5.2.
Let be a -module which is both bounded above and below. Then the natural map
is an equivalence.
Proof of Proposition 5.1 assuming Proposition 5.2.
By assumption (i), it is enough to check that is an equivalence; by assumption (ii), it is enough to check that is an injection; and by assumption (iii) it is enough to check that is an injection.
Again by (i), the map is an equivalence. So, from the diagram
we see that it is enough to check that the vertical maps are injective on homotopy. More generally, we show that whenever is a bounded below -module, the map
is injective. Indeed, by Proposition 5.2 and the fact that the Tate construction commutes with limits of Postnikov towers (see, e.g., [NS18, I.2.6]), we have
Therefore, we need only check that
is injective. Since the maps have increasingly connective fibers, we can replace the left hand side by and reduce to showing that
is injective. Finally, this reduces to showing that the kernel of
consists of elements annihilated by a power of . This is clear because, for each , the system is eventually constant. β
Proof of Proposition 5.2.
Let denote the full subcategory of -modules for which
is an equivalence. Then is stable, closed under retracts, and closed under suspending by representation spheres.
The map is one of -modules, and hence one of -modules, so it must be a retract of
Thus if and only if . So, by replacing with and considering the Postnikov tower, we are reduced to proving the proposition in the case where is a Mackey functor which is a module over .
In particular, is an -module. Let denote the generator of so that . Let be the sub-Mackey functor generated by . This is a finite filtration with associated graded pieces given by Mackey functors with trivial underlying action. So, since is a thick subcategory, we are reduced to the case when is a discrete -module with trivial underlying action.
For the next reduction we recall some notation. If is any Mackey functor, denote by the Mackey functor and, if is an abelian group, denote by the Mackey functor whose transfer map is the identity on and whose restriction map is multiplication by . We also recall that the transfer extends to a map of Mackey functors .
Now consider the two exact sequences
If is any Mackey functor with , then since then is bounded above and hence . Thus, from the exact sequences above, we are reduced to the case where is of the form for an -vector space (with trivial action). Now recall that and hence . So we are reduced to showing that the constant Mackey functor lies in , where is an -vector space with trivial action. This certainly holds for , and in general we have
since geometric fixed points commutes with colimits, and
by direct calculation. (Notice this holds even when is infinite-dimensional). This completes the proof. β
6 Proof of the main theorem
We are now ready to prove the main theorem. Recall that we have constructed classes
and shown that and . With notation as in the introduction, let
and
Then, choosing nullhomotopies which witness , we get a map:
The main theorem is then the statement:
Theorem 6.1.
The map is an equivalence.
Proof.
Combine Proposition 5.1 with the two lemmas below. β
Lemma 6.2.
The map is an underlying equivalence.
Proof.
First observe that, by our construction in the proof of Lemma 4.4, the map restricts to the map , since the nullhomotopy witnessing was chosen to restrict to the nullhomotopy chosen for that came from the already chosen nullhomotopy of . The upshot is that the map
restricts on underlying spectra to the map
obtained just from the relation and extended via the multiplicative structure.
In particular, on mod homology induces a ring map
We know that maps to and that , so that . Modulo decomposables, is the only element whose Bockstein is . So must map to , mod decomposables. It follows that is a mod equivalence, and hence an equivalence. β
Lemma 6.3.
and are free -modules, finite-dimensional in each degree, and isomorphic as graded vector spaces over .
Proof.
If is any -spectrum, then
is a free -module. Applying this in the cases and , we see that each is a free , evidently finite-dimensional in each degree. So it suffices to prove that
as graded vector spaces. Notice that we can write, as graded vector spaces,
where and . Indeed, , on geometric fixed points, gives rise to two classes; one we are calling and the other we are calling . Similarly, , on geometric fixed points, gives rise to two classes: one we are calling and the other , in their usual degrees. The relations are the ones needed to ensure that the monomials not arising from geometric fixed points of elements in are omitted.
It follows that we have an isomorphism of graded vector spaces
We are trying to show that this is isomorphic, as a graded vector space to
We may regard each vector space as a module over in the evident way, and hence reduce to showing that the two vector spaces
and
are isomorphic. (Here recall that , , and ).
Let range over sequences with , range over sequences with , range over sequences with , and let range over sequences with . We impose the following requirements on these sequences:
-
β’
Each sequence has finite support.
-
β’
If , then . (So is otained from by changing some subset of s to s).
-
β’
. That is: and have disjoint support and and have disjoint support.
Then has a basis of monomials
and has a basis of monomials
where . These have the same number of basis elements in each dimension, so . β
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