An effective proof of the Cartan formula: the even prime
Anibal M. Medina-Mardones

TL;DR
This paper provides a constructive proof of the Cartan formula at the cochain level over _2, applicable to general algebras over the Barratt-Eccles operad, including singular cochains of spaces.
Contribution
It introduces an explicit, natural coboundary construction that verifies the Cartan formula at the cochain level for _2-cohomology.
Findings
Constructs a natural coboundary for the Cartan formula at the cochain level.
The proof applies to algebras over the Barratt-Eccles operad.
Works for singular cochains of topological spaces.
Abstract
The Cartan formula encodes the relationship between the cup product and the action of the Steenrod algebra in -cohomology. In this work, we present an effective proof of the Cartan formula at the cochain level when the field is . More explicitly, for an arbitrary pair of cocycles and any non-negative integer, we construct a natural coboundary that descends to the associated instance of the Cartan formula. Our construction works for general algebras over the Barratt-Eccles operad, in particular, for the singular cochains of spaces.
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An effective proof of the Cartan formula: the even prime
Anibal M. Medina-Mardones
Laboratory for Topology and Neuroscience, École Polytechnique Fédérale de Lausanne, Switzerland
Department of Mathematics, University of Notre Dame du Lac, Notre Dame, IN, USA
Abstract.
The Cartan formula encodes the relationship between the cup product and the action of the Steenrod algebra in -cohomology. In this work, we present an effective proof of the Cartan formula at the cochain level when the field is . More explicitly, for an arbitrary pair of cocycles and any non-negative integer, we construct a natural coboundary that descends to the associated instance of the Cartan formula. Our construction works for general algebras over the Barratt-Eccles operad, in particular, for the singular cochains of spaces.
1. Introduction
Let be a space. In [Ste47], Steenrod introduced formulae to define his famous Steenrod squares
[TABLE]
and in [SE62], he axiomatically characterized them by the following:
is natural, 2. 2.
is the identity, 3. 3.
for , 4. 4.
for with , 5. 5.
.
Axiom 5., known as the Cartan formula, is the focus of this work.
To describe our viewpoint and present the contributions of this paper in context, let us revisit some of the history of Steenrod’s construction.
In the late thirties, Alexander, Whitney, and Čech defined the ring structure on cohomology
[TABLE]
using a cochain level construction
[TABLE]
dual to a choice of simplicial chain approximation to the diagonal inclusion.
Steenrod then showed that is commutative up to coherent homotopies by effectively constructing cup- products
[TABLE]
enforcing its derived commutativity. (Axioms for these and connections with higher category theory can be found in [MM18a] and [MM19]). Then, with coefficients in , Steenrod defined
[TABLE]
This definition of the Steenrod squares makes the Cartan formula equivalent to
[TABLE]
The goal of this work is to effectively construct for any and arbitrary pair of cocycles a natural cochain such that
[TABLE]
Following [May70], we take a more general approach and in doing so we describe a non-necessarily effective construction for any -algebra. We work over a fixed algebraic model of the -operad known as the Barratt-Eccles operad. This model, introduced by Berger-Fresse in [BF04], is equipped with a diagonal map and the natural -algebra structure defined by these authors on the normalized cochains of simplicial sets is suitable for effective constructions.
This paper is part of an ongoing effort spearheaded by Greg Brumfiel and John Morgan to build effective models of classical homotopy-theoretic concepts, see for example [BM16] and [BM18]. Motivation for this especific project came from a question of Anton Kapustin. See [KT17] for an instance where one of our formulae is used in the context of topological phases of matter.
Implementations of the constructions of this paper and of state-of-the-art algorithms for the computation of Steenrod squares and cup- products, as introduced in [MM18d], can be found in the author’s website.
Acknowledgement
We would like to thank John Morgan, Greg Brumfiel, Dennis Sullivan, Anton Kapustin, Mark Behrens, Marc Stephan, and Kathryn Hess for their insights, questions, and comments about this project.
2. Conventions and preliminaries
For the remainder of this paper all algebraic constructions are considered over , the field with two elements.
2.1. Chain complexes and simplicial sets
We denote the category of chain complexes of -modules by . Boundary maps decrease degree and for chain complexes and the set of linear maps is a chain complex with
[TABLE]
Let . We remark that is a chain map if and only if it is a degree [math] cycle. Assume and are chain maps, then is a chain homotopy between them if and only if
[TABLE]
We remark that is a chain map if and only if it is a degree [math] cycle, and that is a chain homotopy between two chain maps and if and only if
[TABLE]
The product of two chain complexes and is defined by
[TABLE]
The category is defined to have an object for every non-negative integer and a morphism for each order-preserving function from to .
For integers , the morphisms
[TABLE]
defined by
[TABLE]
generate all morphisms in .
A simplicial set is a contravariant functor from to the category of sets. We denote the category of simplicial sets by and use the standard notation
[TABLE]
The product of two simplicial sets and is defined by
[TABLE]
The functor of normalized chains
[TABLE]
is defined by
[TABLE]
where .
The functor of normalized cochains is defined by composing with the linear duality functor . Notice that in this definition cochains are concentrated in non-positive degrees.
Remark 1**.**
The singular cochains with -coefficients of a topological space coincide with , where is the simplicial set of continuous maps from standard topological simplices to .
2.2. The Alexander-Whitney and Eilenberg-Zilber maps
The functor of normalized chains does not preserve products, i.e., for a general pair of simplicial sets and there is no isomorphism beetween and . Nevertheless, there is a canonical chain homotopy equivalence between them.
The Alexander-Whitney map
[TABLE]
is defined for by
[TABLE]
and the Eilenberg-Zilber map
[TABLE]
is defined for by
[TABLE]
where the sum is over all pairs of disjoint subsets
[TABLE]
of .
It is well known that the compositions is equal to the identity and that the composition is effectively chain homotopic to the identity. A recursive description for one such chain homotopy was first given in [EML53]. A close formula for it, which we learned from [Rea00] and is credited therein to [Rub91], is given next.
The Shih homotopy
[TABLE]
is defined for to be [math] if and if by
[TABLE]
where and the sum is over all pairs of disjoint subsets
[TABLE]
of with and .
2.3. Group actions and algebras over operads
Let be a group. A -action on an object is a group morphism
[TABLE]
where the group structure on is given by composition.
Let be an operad. (See for example [LV12].) An -algebra structure on an object is an operad morphism
[TABLE]
where the operad structure on is induced from composition of linear maps and transpositions of factors.
Let be an object with a -action or an -algebra structure. We identify the elements of or with their images via or .
2.4. The Barratt-Eccles operad
We review from [BF04] the Barratt-Eccles operad.
For a positive integer let be the group of permutations of elements and
[TABLE]
the usual composition of permutations.
For a positive integer define the simplicial set by
[TABLE]
We consider equipped with the action of given by
[TABLE]
Let
[TABLE]
be defined by applying coordinatewise.
For , let
[TABLE]
be edowed with the induced -action. Define an operadic compositions on by
{\mathcal{E}(r)\otimes\mathcal{E}(s_{1})\otimes\cdots\otimes\mathcal{E}(s_{r})}$${N_{*}\big{(}E(r)\otimes E(s_{1})\otimes\cdots\otimes E(s_{r})\big{)}}$${\mathcal{E}(s_{1}+\cdots+s_{r})}$$\scriptstyle{EZ^{r}}$$\scriptstyle{\bm{\circ}_{\mathcal{E}}}$$\scriptstyle{N_{*}(\bm{\circ}_{E})}
where stand recursively for with .
The resulting operad is referred to as the Barratt-Eccles operad. It is a model in the category for the -operad. That is to say, and, for , is a resolution of by free -modules.
3. Cartan coboundaries for -algebras
3.1. Steenrod cup- products and Cartan coboundaries
Since is an -operad, the orbit complex is an algebraic model for , and is generated as an -module by the orbit of the element
[TABLE]
Definition 2**.**
Let be an -algebra. The cup- product of is the image of in . We use the notation
[TABLE]
A Cartan -coboundary is any map in that satisfies
[TABLE]
Definition 3**.**
The chain maps are defined by
[TABLE]
for any basis element .
Lemma 4**.**
Let be an -algebra. For and we have
[TABLE]
and
[TABLE]
Proof.
For (7) we compute
[TABLE]
For (8) we notice that
[TABLE]
and compute
[TABLE]
as desired. ∎
Lemma 5**.**
Let be a chain homotopy between and satisfying
[TABLE]
Then, for any -algebra and , the map defined by
[TABLE]
is a Cartan -coboundary.
Proof.
By assumption
[TABLE]
so evaluating on we get
[TABLE]
Since \big{(}(12)(34)+\mathrm{id}\big{)}(\alpha\otimes\alpha\otimes\beta\otimes\beta)=0, the equivariance assumption implies
[TABLE]
Evaluating (9) on and using Lemma 4 we obtain
[TABLE]
as desired. ∎
3.2. Statement of the main theorem
We now describe the construction of a chain homotopy as stated in Lemma 5.
The first step of our construction is motivated by the well known fact that two group homomorphisms that are conjugate of each other induce homotopic maps of classifying spaces.
Let us consider the three group inclusions
[TABLE]
of into .
Definition 6**.**
The homomorphisms are defined by
[TABLE]
or, more explicitly, by
[TABLE]
We notice that the maps and are conjugated by in , i.e., for
[TABLE]
Definition 7**.**
Let be the simplicial maps induced from and respectively. Explicitly,
[TABLE]
for any .
We introduce a linear map which, as we will see later, is an appropriately equivariant chain homotopy between and .
Definition 8**.**
Let be the degree linear map defined on basis elements by
[TABLE]
The second step relates the maps and , as well as and . It turns out, as we will see later, that the maps in the first pair are equal, whereas the maps in the second are chain homotopic via an appropriately equivariant map that we now introduce.
Definition 9**.**
Let be the degree linear map defined on basis elements by
[TABLE]
We are ready to state our main result.
Theorem 10**.**
Let be an -algebra. For any the map in defined by
[TABLE]
is a Cartan -coboundary.
3.3. Proof of the main theorem
We will prove Theorem 10 after four lemmas.
Lemma 11**.**
In \mathrm{Hom}\big{(}\mathcal{E}(2),\mathcal{E}(4)\big{)}
[TABLE]
Proof.
The essence of the proof is a telescopic sum argument.
[TABLE]
for any basis element . ∎
Lemma 12**.**
The map satisfies the following form of equivariance:
[TABLE]
Proof.
Let be the degree linear map defined on basis elements by
[TABLE]
Notice that . We will verify (12) by checking it for each . Using (10) we notice that for any in we have
[TABLE]
Therefore,
[TABLE]
for any basis element . ∎
Lemma 13**.**
In \mathrm{Hom}\big{(}\mathcal{E}(2),\mathcal{E}(4)\big{)}
[TABLE]
and
[TABLE]
Proof.
We have
[TABLE]
and
[TABLE]
for any basis element . ∎
Lemma 14**.**
The map satisfies the following form of equivariance:
[TABLE]
Proof.
Since for any
[TABLE]
we have
[TABLE]
for any basis element . ∎
Proof of Theorem 10.
We will show that satisfies the hypothesis of Lemma 5. Notice that the equivariance condition follows from Lemma 12 and Lemma 14. To verify that is a chain homotopy between and we use Lemma 11 and Lemma 13
[TABLE]
as desired. ∎
4. The -algebra structure on normalized cochains
In this section we effectively describe an -algebra structure on the normalized cochains of simplicial sets. This will allow us to apply our construction of Cartan -coboundaries to this central example. Following [BF04], we achive this in two steps corresponding to the two operad morphisms
[TABLE]
Here is the Surjection operad of McClure-Smith [MS03] and Berger-Fresse [BF04], the first arrow is the Table Reduction morphism of [BF04], and the second is the natural -algebra structure introduced in [MS03] and [BF04].
4.1. The Surjection operad
We review the definition of the Surjection operad of McClure-Smith [MS03] and Berger-Fresse [BF04].
For a non-negative integer define
[TABLE]
Fix and consider all . We make the free -module generated by all functions into a chain complex by declaring the degree of to be and its boundary to be
[TABLE]
where is the injective order preserving function missing .
We define to be the quotient of this chain complex by the submodule generated by the functions which are either non-surjective or for which equals for some .
The chain complex carries an action of given by composition. The collection is an operad with partial composition defined on two generators and as follows. Represent the surjections and by sequences and and suppose that appears times in the sequence representing as . Denote the set of all tuples
[TABLE]
by and for each such tuple consider the subsequences
[TABLE]
Then, in , replace the value by . In addition, increase the terms by and the terms such that by . The surjection is represented by the sum, parametrized by , of these resulting sequences.
Example 15**.**
Let us consider
[TABLE]
Then, equals
[TABLE]
where the internal parenthesis are included solely for expository purposes.
4.2. The Table Reduction morphism
We review the definition of the Table Reduction operad morphism
[TABLE]
introduced in [BF04].
Given a basis element we define
[TABLE]
as a sum of surjections
[TABLE]
parametrized by all with each and .
For one such tuple we now describe its associated surjection . Consider the table
[TABLE]
define recursively
[TABLE]
For we identify such that and define to be the -th element in not in
[TABLE]
Example 16**.**
Let us compute TR\big{(}(23),e,(12)(34)\big{)}. Its associated table is
[TABLE]
and the tuples parametrizing the sum correspond to all permutations of . Then,
[TABLE]
4.3. The diagonal and join maps
We review the natural -algebra structure on introduced in [MS03] and [BF04] using the perspective presented in [MM18b]. We notice that this -algebra structure provides with an -algebra structure
[TABLE]
Let be the representable simplicial set . We identify a morphism with its image . As usual, it suffices to describe the -structure for representable simplicial sets only.
Let be defined on basis elements by
[TABLE]
and, for any , let be defined on basis elements by
[TABLE]
We notice that is equal to the composition of the Alexander-Whitney map and the doubling map
[TABLE]
and that is commutative.
We now describe the -algebra structure on . Let
[TABLE]
be a surjection, then is defined by
[TABLE]
where is recursively defined by
[TABLE]
and is given by applying to the factors in positions .
Remark 17**.**
This -algebra structure on normalized cochains of simplicial sets is induced, as explained in [MM18c], from an explicit cellular -bialgebra structure on the geometric realization of .
Appendix A Explicit examples
Let be the -th representable simplicial set and denote by . In this appendix, we will compute for an arbitrary pair of homogeneous cocycles the value
[TABLE]
in terms of and . We will restrict to and the smallest integer for which this value is not identically [math].
Recall that
[TABLE]
and that our Cartan -coboundary is defined by
[TABLE]
where is the Table Reduction morphism and
[TABLE]
[TABLE]
We remark that the cochain witnesses the relation
[TABLE]
where and are the degrees of and .
Example 18**.**
For , we have
[TABLE]
and
[TABLE]
Therefore,
[TABLE]
and
[TABLE]
Example 19**.**
For , we have
[TABLE]
and
[TABLE]
Therefore,
[TABLE]
and
[TABLE]
Example 20**.**
For , we have
[TABLE]
and
[TABLE]
Therefore,
[TABLE]
and
[TABLE]
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[BF 04] Clemens Berger and Benoit Fresse. Combinatorial operad actions on cochains. In Mathematical Proceedings of the Cambridge Philosophical Society , volume 137, pages 135–174. Cambridge University Press, 2004.
- 2[BM 16] Greg Brumfiel and John Morgan. The pontrjagin dual of 3-dimensional spin bordism. ar Xiv preprint ar Xiv:1612.02860 , 2016.
- 3[BM 18] Greg Brumfiel and John Morgan. Quadratic functions of cocycles and pin structures. ar Xiv preprint ar Xiv:1808.10484 , 2018.
- 4[EML 53] Samuel Eilenberg and Saunders Mac Lane. On the groups H ( π , n ) 𝐻 𝜋 𝑛 {H}(\pi,n) , I. Ann. of Math.(2) , 58(1):55–106, 1953.
- 5[KT 17] Anton Kapustin and Ryan Thorngren. Fermionic spt phases in higher dimensions and bosonization. Journal of High Energy Physics , 2017(10):80, 2017.
- 6[LV 12] Jean-Louis Loday and Bruno Vallette. Algebraic operads , volume 346 of Grundlehren der Mathematischen Wissenschaften [Fundamental Principles of Mathematical Sciences] . Springer, Heidelberg, 2012.
- 7[May 70] J Peter May. A general algebraic approach to Steenrod operations. In The Steenrod Algebra and its Applications: a conference to celebrate NE Steenrod’s sixtieth birthday , pages 153–231. Springer, 1970.
- 8[MM 18a] Anibal M. Medina-Mardones. An axiomatic characterization of Steenrod’s cup- i 𝑖 i products. ar Xiv preprint ar Xiv:1810.06505 , 2018.
