of Matroids
Abstract.
Using the geometric realization spectral sequence and the Serre spectral sequence, we compute , the first K-theory group of the proto-exact category of pointed matroids, answering a question of Jun, Sistko and Wright.
Contents
1. Introduction
Matroids are combinatorial objects which abstract and encode the notion of independence, including linear independence within vector spaces and the absence of cycles in a finite graph. As such, they play a prominent role in various fields ranging from combinatorics and discrete mathematics to optimization and algebra. Also in the field of tropical geometry, which studies algebraic varieties from a combinatorial/linearized perspective, matroids are ubiquitous. They have in particular been used by Engel, de Gaay Fortman and Schreieder in [9] to obtain interesting results in algebraic geometry, such as the stable irrationality of very general cubic threefolds and the failure of the integral Hodge conjecture for very general principally polarized abelian varieties of dimension at least .
Algebraic -theory is a powerful tool from homotopy theory which, in its simplest description, studies decompositions of objects. In recent years, the application of this tool to combinatorial objects has received increasing attention. The starting point of this was Zakharevichβs work on the scissors congruence -theory of assemblers [24] and [25]. Her constructions associate -theory spectra and hence -theory groups to suitable categories equipped with scissors congruence/cutting and pasting operations, recovering, for instance, classical scissors congruence groups and the Grothendieck ring of varieties from algebraic geometry. The higher -groups provide further invariants of decomposition problems and are an active field of study. For example, recent work of Kupers, Lemann, Malkiewich, Miller and Sroka [15] relates scissors congruence -theory to the homology of scissors automorphism groups, providing a group-theoretic interpretation of these higher invariants. The authors describe as the abelianization of scissors automorphism groups and as such further illustrate how combinatorial -theory connects decomposition relations with the symmetries which preserve them.
The -theory of the category of pointed matroids , as first considered in [10], is part of this development. The relevant decompositions stem from restrictions of a matroid together with their complementary contractions . In [10], the authors show that these notions equip the category with the structure of a proto-exact category, which is a not necessarily additive variant of exact categories. By [6], this is one of the frameworks which enable -theory. The resulting algebraic -theory of pointed matroids hence studies and encodes restriction-contraction decompositions of matroids.
Currently, not much about the homotopy groups of , that is, about the -groups of pointed matroids, is known. Eppolito, Jun and Szczesny showed in [10] that and that the stable homotopy groups of spheres embed into the -groups: . In particular, the -groups contain interesting information of a homotopical nature, but how much more information do the -groups contain? This is exactly what Jun, Sistko and Wright ask in Remark 5.6 of [14]. Our main result answers this question in degree one:
Theorem (Theorem 4.15).
There is an isomorphism .
In particular, the only information comes from the first stable homotopy group of spheres.
Our main tool is the geometric realization spectral sequence for homology. It expresses the relevant homology groups in terms of automorphisms of matroids and their flags, and we use two key ideas to get a hold of these groups. The first one is that we can use so-called free coextensions of matroids to raise the rank of a matroid without changing its corresponding automorphism class in the relevant term of the spectral sequence. This allows us to assume that all pointed matroids are free and hence that they are basically nothing but finite pointed sets. The second one is to use suitable successive decompositions into matroids with one element and then to study these decompositions into simple pieces to find generators. This allows us to compute the second homology of the delooped K-theory space of pointed matroids. To put everything together, we use the Serre spectral sequence, which allows us to relate this homology group to the desired homotopy group, resulting in the above computation. Based on our arguments, we give the following conjectural description of the entire -theory spectrum:
Conjecture (Conjecture 4.16).
The map induced by the rank map and by the forgetful map to pointed finite sets is an equivalence of spectra. In particular, we have isomorphisms for all positive .
This article is structured as follows. Section 2 introduces and collects relevant facts about matroids and their pointed versions. Section 3 briefly reviews proto-exact categories and their K-theory, including the aforementioned description in terms of flags of matroids. Finally, Section 4 is dedicated to the computations with the geometric realization and Serre spectral sequences and concludes with the main result and the conjectural description from above.
Acknowledgements. The author wishes to thank Ming Ng for making him aware of the problem of computing the -theory of matroids, specifically in degree . Furthermore, the author used ChatGPT 6-Astra for proofreading and to search for references. Except for pointing out typos and the like, it found combinatorial slipups in the proof of Proposition 4.10 and fixed them.
2. The Category of Matroids
In this section we give a quick introduction to matroids and generally refer the reader to [19] or [23] for more information. Despite this, we will provide arguments for a few standard lemmas to get more homotopically minded readers used to the combinatorial notions.
Matroids are combinatorial objects which abstract the notion of linear independence from vector spaces. There are various equivalent definitions, of which we will use and present three. As in [10], the one in terms of flats will be the most relevant one for this article.
Definition 2.1.
A matroid is a pair consisting of a finite set , called the ground set of the matroid , together with a collection of independent subsets subject to:
- (i)
The empty set is independent, i.e., we have .
- (ii)
The set is hereditary, i.e., if and , then .
- (iii)
The set satisfies the Steinitz exchange property, that is, whenever with , then there exists an element such that .
As in linear algebra, any maximally independent set is called a basis of the matroid and the size of any two bases agrees; see Lemma 1.2.1 of [19]. This number is called the rank of the matroid and is denoted by . More generally, the rank of any subset of a matroid is defined as the size of the largest independent set contained in .
Before we get to some central examples, let us introduce two further notions.
Definition 2.2.
Let be a finite set. A closure operator on is a map subject to:
- (i)
The map is extensive, i.e., for all subsets , we have .
- (ii)
The map is idempotent, i.e., we have for all subsets .
- (iii)
The map is monotone, i.e., for all subsets with we have .
If additionally for all subsets and all , whenever , we have , we say that the closure operator satisfies the Steinitz exchange property (SEP).
To state the definition of flats, let us quickly clarify the notion of cover used here. Given two subsets and of some finite set , we say that covers , if and there is no subset with . In other words, covers if is minimal among subsets of which properly contain .
Definition 2.3.
Let be a finite set. A collection is a set of flats on , if it satisfies the following axioms:
- (i)
The set is a flat, i.e., is contained in .
- (ii)
The set of flats is stable under finite intersections, i.e., we have for all .
- (iii)
For all flats , the set is a partition of .
A basic result of matroid theory now identifies all those notions:
Proposition 2.4.
Given a finite set , the following data are equivalent:
- (i)
A matroid with ground set ;
- (ii)
A closure operator on satisfying the Steinitz exchange property;
- (iii)
A set of flats on .
While we do not want to present a proof of this standard fact, for which we refer the reader to Corollary 1.4.7 and Exercise 11 in Section 1.4 in [19], we do want to indicate how to pass between these notions:
While this is relevant in matroid theory, it will actually not be of importance for this article to know how to pass between these equivalent characterizations of matroids. We only need to know that we can verify that two matroids agree by choosing one of the three notions, which gives us quite some flexibility.
Let us finally present a few examples, some of which we will make use of later on.
Example 2.5.
- (i)
A vectorial matroid has a finite subset of a vector space as ground set and the independent sets are given by linearly independent sets within . The closure operator maps a subset to the set of all vectors in lying in the linear span of , and the flats of a vectorial matroid are those subsets with .
- (ii)
A graphic matroid has the edges of a finite graph as ground set and the independent sets are the forests, i.e., those collections of edges such that there is at most one path between any two of their vertices. The closure operator maps a subset to the set of all edges connecting vertices already connected by paths in , and the flats of a graphic matroid are those subsets that contain all paths staying entirely within the connected componentβs set of vertices.
- (iii)
Given non-negative integers and with , the uniform matroid on a finite set with elements has every subset of cardinality at most as an independent subset. The closure operator maps subsets of cardinality smaller than to themselves and subsets of cardinality at least to , and the flats are the subsets of cardinality smaller than and itself. Note that it is customary to denote this matroid by independently of the ground set.
- (iv)
As a notable special case of the previous example we have the free matroid on , which is the uniform matroid . Here every subset is independent, the closure operator is just the identity map, and every subset is a flat.
Now we come to the notion of morphisms between matroids. While there are multiple meaningful choices, the most common one is the following.
Definition 2.6.
A map between two matroids is strong if is a flat of for every flat .
Example 2.7.
In the setups from linear algebra and graph theory, strong maps arise as expected:
- (i)
If and are two vectorial matroids with respect to subsets and from two vector spaces and over a field , then any linear map satisfying yields a strong map by restriction.
- (ii)
If and are two graphic matroids associated with graphs and , then any graph morphism yields a strong map .
Matroids together with strong maps form a category , as is not difficult to verify. Its properties are for instance studied in the article [13]. Let us note here that a bijective strong map between matroids of the same rank is already an isomorphism, which follows from Corollary 7.3.4 together with Proposition 7.3.6 of [19]. In particular, a bijective strong self-map is an automorphism.
There are various operations on matroids which are crucial for this article, some of which yield the decompositions of matroids which the -theory studies. Let us introduce those:
Definition 2.8.
Let be a matroid with ground set and let be a subset of .
- (i)
The restriction of to is the matroid with ground set and
- -
independent sets
- -
closure operator
- -
flats
- -
- (ii)
The contraction of with respect to is the matroid with ground set and
- -
independent sets for a fixed basis of
- -
closure operator
- -
flats
- -
The restriction to the complement of is also called the deletion of and denoted by .
These notions have some compatibility, as the following simple lemma shows, which can be found as Proposition 3.1.25 (iii) in [19].
Lemma 2.9.
Let be a matroid and let and be subsets of with . Then we have .
Proof.
First note that both of these matroids have ground set . Now choose a basis of . This is then also a basis of . Now we have by definition that a subset is independent in if and only if is independent in , which is equivalent to being independent in as . Moreover, this last condition is equivalent to being independent in , which finishes the proof. β
The category of matroids admits finite coproducts, defined as follows.
Definition 2.10.
The direct sum of two matroids and is the matroid with ground set and
- -
independent sets
- -
closure operator
- -
flats
A central operation for us will be the free coextension of a matroid by a single element.
Definition 2.11.
Let be a matroid with ground set and let . The free coextension of by is the matroid with ground set and
- -
independent sets
- -
closure operator mapping a subset to if is contained in and is independent, and mapping it to otherwise
- -
flats
Based on the above description of the independent sets we immediately obtain . Furthermore, the above definitions are made to satisfy the following.
Lemma 2.12.
Let be a matroid with ground set and let . Then we have and . If is non-free, we furthermore have and if is free, then .
Proof.
We verify the first claim in terms of the closure operator. Here we have
for all subsets , so that .
For the second claim, note that since , we have and thus . In particular, is free on .
Now suppose that is not free, so that is a dependent set of . Then
and we obtain . If is free instead, then is an independent set of and we get
so that . This finishes the proof. β
Moreover, automorphisms of matroids can be extended to free coextensions, which will become very useful in our -theory computations later on. This statement follows from Proposition 7.2.6 and Proposition 7.3.9 of [19], but their proofs use notions we have not introduced here. Therefore, we will give a direct proof for the convenience of the reader.
Lemma 2.13.
Let be a matroid and let be the free coextension of by . If is an automorphism, then so is its extension defined by mapping to .
Proof.
Since the map is clearly bijective, it suffices to verify that it is strong, as we observed just below Example 2.7. By definition, a flat of is either an independent set or for some flat . In the first case the preimage is independent and hence a flat of , and in the second case is also a flat of . So is strong and thus an automorphism. β
Let us note that the above statement is false for endomorphisms, as can be easily seen from constant maps between uniform matroids.
To define pointed matroids, we call an element a loop if it is not contained in any independent set of the matroid . Equivalently, is a loop if it is contained in the unique minimal flat of . As such, loops play the role of the zero vector in vector spaces.
Definition 2.14.
A pointed matroid is a pair where is a matroid and is a loop of .
As is done in topology, we usually omit the base point from the notation. However, we will need to distinguish the ground set and its reduced variant .
Example 2.15.
In the pointed setting, we add a distinguished loop to uniform matroids. In particular, and . This makes the zero matroid, and free pointed matroids are those matroids that are free after removing the base point; see also Section 4.2 of [13].
Definition 2.16.
A map between two pointed matroids is strong if and is a flat of for every flat .
This gives rise to a category , the category of pointed matroids, which is studied in more detail in [13]. Here it is also verified that this category admits a forgetful functor and has finite coproducts called direct sums, which we recall as part of the following list, which mostly stems from Remark 2.9 of [10]:
Remark 2.17.
For a pointed matroid and a subset we adopt the following conventions regarding the various operations that we have introduced in the unpointed setting:
- -
The restriction is the unpointed restriction including the base point. In particular, the restriction of an automorphism acts (trivially) on the base point.
- -
The contraction is the usual unpointed contraction . The base point is not allowed to be contracted.
- -
The direct sum of with another pointed matroid is the usual unpointed direct sum with the two base points identified. In other words, the ground set is with base point , and the independent sets and flats are disjoint unions of independent sets and flats of the two matroids, with the base points identified for the flats.
- -
The free coextension of by an element is the usual unpointed free coextension with the base point added as a loop . Here the deletion is in the unpointed setting.
With those conventions in place, Lemma 2.12 and Lemma 2.13 also hold in the pointed setting with replaced by , as can be quickly verified. Therefore, we will also refer to those statements when we use them in the pointed setting.
Example 2.18.
Let us conclude this section with two central examples of pointed strong maps, also found as Example 2.11.3 of [10]:
- (i)
Inclusion maps of the form are by definition pointed strong maps.
- (ii)
Quotient maps of the form are by definition pointed strong maps. Here all the elements contained in are mapped to the base point.
These types of maps rise to the exact sequences encoded in the categorical structure of the next section.
3. Proto-exact Categories and their K-theory
Following Dyckerhoff and Kapranov [6], we give a brief recollection of proto-exact categories, which are not necessarily additive variants of exact categories, and of the -construction of K-theory for such categories. This yields the algebraic K-theory space of pointed matroids.
Definition 3.1.
A proto-exact category is a category together with two collections of morphisms and , called admissible monomorphisms and admissible epimorphisms, respectively, subject to:
- (i)
The category has a zero object , and any morphism of the form lies in and any morphism of the form lies in .
- (ii)
The collections and contain all isomorphisms and are closed under composition.
- (iii)
A commutative square
with horizontal morphisms from and vertical morphisms from is cartesian if and only if it is cocartesian.
- (iv)
Any diagram in of the form
orβ
with horizontal morphisms from and vertical morphisms from can be completed to a bicartesian square as in the previous point.
Admissible monomorphisms are typically denoted by and admissible epimorphisms by , despite the fact that those symbols could also stand for monomorphisms and epimorphisms in the category . A bicartesian square of the form
is usually denoted by and is called an admissible exact sequence of .
A natural question is, of course, how exactly proto-exact categories relate to their classical counterpart.
Remark 3.2.
For a proto-exact category to be exact, we would need to require to be additive instead of just being pointed, to be closed under all pushouts and not only under pushouts along , and to be closed under all pullbacks and not only under pullbacks along . For more details on this comparison, we refer the reader to Section 1 of [17].
Example 3.3.
There are two central examples of interest to us here:
- (i)
The category of pointed finite sets is a proto-exact category. Here the admissible monomorphisms are the injections and the admissible epimorphisms are those surjections whose fibers over non-base points are singletons; see Example 2.4.4 (a) of [6].
- (ii)
The category of pointed matroids is a proto-exact category, as shown in Section 5 of [10]. Here consists of inclusions of the form up to isomorphism and consists of quotient maps up to isomorphism, where in both cases .
As explained in Remark 3.2, exact categories are examples of proto-exact with the same exact structure. For examples from quadratic form theory or Arakelov geometry, we refer the reader to Section 2.4 of [6], and for examples related to -geometry, we refer the reader to [7].
Let us now turn our focus towards K-theory. Originally, Waldhausenβs -construction applies to categories with weak equivalences and cofibrations, nowadays usually referred to as Waldhausen categories [20]. As explained in Section 2.4 of [6], it is also available for proto-exact categories. Let us recall the construction.
For a non-negative integer , we consider the functor category which corresponds to the poset of ordered pairs with the order if and . Then defining a functor amounts to a choice of a commutative diagram in of the form
If now is a proto-exact category, we let denote the maximal subgroupoid of the full subcategory of those functors satisfying
- (i)
for all ;
- (ii)
The horizontal arrows are admissible monomorphisms and the vertical arrows are admissible epimorphisms;
- (iii)
All squares are bicartesian.
This construction comes with face and degeneracy maps by omitting the -th row and -th column or inserting an additional row and column at the -th position via identity maps. It is then not difficult to verify that one obtains a simplicial groupoid .
Dyckerhoff and Kapranov provide another description of the groupoids , which we make use of. For this, we let denote the groupoid of chains of composable admissible monomorphisms
and their isomorphisms. We refer to this as the groupoid of flags of length . Note that this makes the terminal groupoid.
Lemma 3.4.
Let be a proto-exact category. For all positive integers , the functor mapping a diagram to the subdiagram
is an equivalence of groupoids. Under these equivalences, the face maps are identified with
- (i)
the map that omits the -th entry for all ;
- (ii)
the map that sends a flag
of length to the flag of quotients
for .
Proof.
The equivalence has been established in Lemma 2.4.9 (i) of [6]. For , the description of the face maps is clear from the definition of . Thus it only remains to understand the case of . Applying to a diagram leaves
as the new first row. Now we want to identify this row in terms of the old first row. Since all the squares in are bicartesian, we have pushout squares of the form
for all by composing the squares horizontally. In particular, we obtain isomorphisms , yielding the claimed description of the face maps also for . β
In the setting of Waldhausen categories, this lemma is also known, as the reader might expect. It can be found as Definition IV.8.3.1 in Weibelβs -book [22] together with the paragraph immediately following it. As it is quite crucial for Section , we still wanted to include the short argument dewcribing the face maps.
In the case of matroids, we will often abbreviate a flag
as or and denote its isomorphism class by . Moreover, we call a flag proper if is non-empty and all other inclusions are proper inclusions.
Now that we have this model for , let us define the K-theory space. For this, we consider the simplicial space obtained by applying the classifying space functor.
Definition 3.5.
The (delooped) algebraic K-theory space of a proto-exact category is the geometric realization of the simplicial space , and its shifted homotopy groups are the algebraic K-theory groups .
Technically, this should of course not be called the algebraic K-theory space, as this is a delooping of it, but for the sake of simplicity, we will still refer to it as such. As for other types of categories, this is not only a space, but actually carries additional structure.
Lemma 3.6.
The space is the infinite loop space of a spectrum . In particular, it becomes a connected -space on the level of the homotopy category.
Proof.
Since has finite coproducts, this can be shown exactly as for exact categories, where it is a standard fact. We refer the reader to [1] for a modern treatment of this fact for the -construction, and to the proof of Theorem 3.5.3 of [12] for a write-up of the equivalence of - and -constructions in the setting of proto-exact categories. β
The more combinatorially minded readers, who might not necessarily be familiar with the notions of the above lemma, need not worry. This lemma will be used exactly once, at the end of section , and all we need from it is that the fundamental group of the delooped -theory space acts trivially on the second homotopy group, which is true for these so-called -spaces.
Finally, let us note that the -theory and Grothendieck-Witt theory of proto-exact categories was also studied by Eberhardt, Lorscheid and Young in [8].
4. Computing the K-theory of Matroids
In Theorem 6.3 of [10], the authors compute , using a description of for proto-exact categories with finite coproducts as the free abelian group of isomorphism classes of matroids, up to βmaking short exact sequences splitβ. This is the usual definition of the Grothendieck group. Their result can be stated as follows:
Theorem 4.1 ([10]).
The map is an isomorphism.
Moreover, using the free-forgetful adjunction between and from [13], the authors establish the following result as Theorem 6.4 of loc. cit.β
Theorem 4.2 ([10]).
There are injective group homomorphisms for all non-negative integers .
Putting these two theorems together, we see that at least for , the K-theory of matroids is not determined by the homotopy of the sphere spectrum. But this does raise the question of what happens in other degrees, as Jun, Sistko- and Wright ask in Remark 5.6 of [14]. Our goal for this section is to give a full answer in degree and, based on that, give our prediction about the remaining cases of .
Throughout this section, all matroids are pointed, all strong maps preserve the base point (including automorphisms of matroids), and we let denote the (delooped) K-theory space of pointed matroids. As seen in the previous section, it is given as the geometric realization , and its homotopy groups are the algebraic K-theory groups of pointed matroids.
The main tool we will be using is the homological geometric realization spectral sequence
For this entire section, unless we explicitly state otherwise, whenever we write for some integers , and , we mean the terms of this spectral sequence. Here the differentials are given as the maps induced by the alternating sum over the face maps. For a detailed exposition of this spectral sequence, we refer the reader to Section 12.6.1 of the book project [16].
The basic idea is to obtain enough information about via the above spectral sequence and then use the Hurewicz map to compare with .
The first group we wish to compute is . To have a better understanding of it, let us start by giving a presentation in terms of automorphisms.
Proposition 4.3.
The group is isomorphic to the quotient group
where runs over all isomorphism classes of matroids .
Proof.
First note that since is a point, we have and thus . Thus it suffices to determine those two groups making up this quotient. Lemma 3.4 tells us that the first one is
where runs over all isomorphism classes of matroids . By the same reasoning, we obtain
where runs over all isomorphism classes of flags of length . By another application of Lemma 3.4, the three face maps send a flag to the matroids
On the level of automorphisms, these induce the group homomorphisms
-
, ,
-
, ,
-
,
where acts on by the same underlying permutation as . In particular, the differential is given by
for an element . This proves the claim. β
This group might look familiar to the reader. For an exact category , this group is also known as Bassβ . It comes equipped with a natural map , but this map need not be an isomorphism. For more on this group we refer to [2], [3], [11] or to the introduction of [18].
To compute explicitly, we will make use of the following lemma.
Lemma 4.4.
There is a well-defined group homomorphism mapping the class of an automorphism to the sign of the underlying permutation of .
Proof.
Let be a matroid with ground set of cardinality . As is a subgroup of , we get a sign map by restricting the one on . Now we factorize it through the abelianization and obtain a homomorphism by taking the direct sum of those maps, which by abuse of notation we still denote by . Finally, we check that this sign map factorizes through the quotient with respect to the image of . For this let and let with . Then also preserves , which gives rise to and . Now we factor each of these permutations into transpositions, say and , and extend them to by letting them act as the identity outside of their respective domains. This gives a factorization of into transpositions and results in
Therefore, the sign map respects the relations from and we obtain the desired sign map on . β
Theorem 4.5.
We have .
Proof.
By Proposition 4.3, the group agrees with the quotient group
To compute it, we show that any automorphism of a matroid may be exchanged for the same underlying permutation on the free matroid on . For this suppose is not a free matroid, i.e., . We consider the free coextension of by a new element and use Lemma 2.13 to extend to an automorphism of fixing . By Lemma 2.12, this yields the relations
and
from which we obtain . Since those two matroids have the same ground set and we have , we can iterate this process until agrees with the class of its underlying permutation on the free matroid on . Now we consider a permutation . Since is generated by transpositions, we can write for some transpositions and obtain
Therefore, it suffices to understand the class of transpositions. If is any transposition, the defining relations of give us
So all transpositions define the same class in . In particular, by what we have shown so far, the entire group is generated by . Since
we thus have or . The former cannot be the case, as we can detect the non-triviality of the transposition via the sign homomorphism from Lemma 4.4. Thus we have shown that . β
What the above proof really does is show that we can increase the rank of any matroid until it is full without changing the associated class. Afterwards, we only need to work out the remaining combinatorics on the level of finite sets and their permutations, resulting in the desired computation.
Next we will deal with the group . By definition, we have
where those direct sums run over all isomorphism classes of flags of lengths , or . As in the proof of Proposition 4.3, the differentials can be computed as
by using Lemma 3.4, which results in the following presentation.
Proposition 4.6.
The group is isomorphic to the quotient of the subgroup
by the group generated by
for all matroids and all flags of length .
Actually, this presentation can be simplified a bit, which we will make use of:
Lemma 4.7.
In the above presentation, we may restrict to proper flags both for the generators and for the relations.
Proof.
Let be a matroid. The two non-proper generators associated with are and . Since
and
these are identified with for any matroid . In particular, any cycle satisfies
for a -linear combination of classes of proper flags and some integer . As , the right-hand side is a cycle. Hence
But for a proper flag , none of the terms , or can be as the respective reduced ground sets are all non-empty. This forces , so that is a cycle made out of classes of proper flags representing the same class as .
For the three kinds of non-proper flags of length we have
So the images under of classes of non-proper flags only make use of non-proper flags, and similarly, images under of classes of proper flags only involve proper flags. If a cycle built from proper flags lies in the image of , we write it as
where is made up of classes of proper flags and is made up of classes of non-proper flags. By the above computations, so are the respective images and we obtain by comparing coefficients. In particular, all relations between classes built from proper flags arise from images of classes of proper flags, finishing the proof. β
We will show that the group is cyclic of infinite order, i.e., that it is isomorphic to . For this, let us already define the element that will turn out to be a generator of . It is the element
where denotes the reduced ground set of the matroid . Here is a loop, that is, it is not contained in any independent set, while is an independent set. We quickly verify that indeed gives rise to an element in .
Lemma 4.8.
The element defines an element in .
Proof.
We apply the differential and obtain
so that yields a class . β
So we have a special element to work with. Next we need to figure out how to relate it to elements . For this we observe that we can reduce the size of using the relations stemming from the differential . Picking an element , we get
Here the first and the last terms make use of singletons and are hence a lot simpler, and the term in the middle also uses a subset of smaller size. Therefore, we can iterate this for the middle term, resulting in rather simple terms after enough iterations. Thus it makes sense to group all the singleton terms arising in this process, which we will do now. For any isomorphism class of matroids we choose a representative together with an ordering of its reduced ground set. This allows us to define a group homomorphism
by mapping a basis element to if and to if . As we chose an ordering of the , we now investigate how much the map depends on this ordering.
Proposition 4.9.
For any permutation , we have
Proof.
If consists of two elements and , the defining formula of directly yields
We will now show that this is true more generally when swapping only the first two elements of for any matroid , at least when working mod . For this we let be a matroid with and swap with . Then we have
since the swap does not matter once both and have been contracted. In particular, we obtain
Using the explicit formula for the differential , we see that in the quotient , the first two summands agree with
and the latter two summands agree with
Thus we have
as claimed above. Exchanging two adjacent at a later position leaves earlier and even later summands unchanged, because the respective contracted sets agree. Only the exchanged elements contribute to the difference, computed as above. Since , matroids of this form must be isomorphic to one of the matroids
For the first three, swapping the two elements is an automorphism, which hence results in no difference. For , the difference is by definition given by . As any permutation can be written as a product of adjacent transpositions, this yields
which is what we wanted to show. β
Due to this proposition, we will allow ourselves to write instead of as long as we work mod . As the motivation for the map hinted at, these kinds of elements allow us to express the class of a flag in terms of , its restriction to and its contraction with respect to as follows.
Proposition 4.10.
For any matroid and any non-empty proper subset , we have
Proof.
For a proper flag , we choose an ordering so that the elements of the subset come first, where . Now we claim that
We consider the proper flag
for all . Its image under is given by the sum of
and
where we made use of Lemma 2.9. Summing the first two summands over all gives
so that we obtain
after adding the sum . Finally, we have
which yields the claimed formula. β
Theorem 4.11.
We have .
Proof.
As we have mentioned already, we claim that generates the group . To verify this, we let be a cycle of proper flags. Then the previous proposition yields
mod . In particular, we have mod for a suitable . In other words, generates the group . It remains to show that has infinite order. For this we define a group homomorphism
by mapping a basis element to , and denote its restriction to by . Since for any generator , we have
we get an induced homomorphism . It maps to
so that the order of is infinite. This finishes the proof. β
Remark 4.12.
Although we do not want to get into detail, let us quickly note how the homomorphism used in the proof of Theorem 4.11 arises. There is a natural homomorphism which maps a flag to the class of its successive quotients in
Evaluating the cup product of the rank and reduced cardinality maps viewed as representatives of elements in on these classes then yields up to a sign; see the explicit formula at the top of page 110 of [4] for .
Based on the previous results, we have almost all the needed ingredients to compute the group . To complete this computation, we will compare two short exact sequences, the first one being:
Corollary 4.13.
There is a short exact sequence of abelian groups of the form
In particular, we have a splitting .
Proof.
First note that the line vanishes for positive since is the terminal groupoid. In particular, we have and hence . Moreover, we have and by Theorem 4.5 and Theorem 4.11. For degree reasons, no non-trivial differential can enter at the position for and the only potentially non-trivial differential leaving this position for is . As the line vanishes for positive , the differential is the zero map. Therefore, . Analogously we obtain
for degree reasons. This yields the filtration
with subquotients given by:
-
,
-
,
-
.
Therefore, the short exact sequence
shows the claim. β
In other words, the second homology of the K-theory space is either or . As we are interested in the K-groups, that is, in the homotopy of the K-theory space, we now want to compare this homology group with .
Proposition 4.14.
There is a short exact sequence of abelian groups of the form
In particular, we have a splitting .
Proof.
From obstruction theory we have the fiber sequence
where denotes the universal covering of , and we can hence consider the associated homological Serre spectral sequence
To avoid confusion, let us explicitly state that the following terms refer to this spectral sequence. Part of its low-degree exact sequence is given by
but since is simply connected, we have , so the outer two terms vanish. In particular, the map in the middle is an isomorphism.
Now we want to determine . For this we first note that the line at vanishes due to being trivial. This immediately yields
and
For degree reasons, no other potentially non-trivial differential enters or leaves the -position on higher pages. Thus we get
Now we splice this into the above exact sequence as follows:
By Theorem 6.3 of [10], we know that and hence that is a torus. In particular, and . Next we use that the Hurewicz map is -equivariant, so that we obtain
Finally, becomes a connected -space by Lemma 3.6, so the action of on is trivial and we are done. β
With a tiny bit more care, the map in the above short exact sequence can be seen to be the Hurewicz map, but we do not need this. Now we can put everything together and obtain the desired computation:
Theorem 4.15.
We have .
Proof.
Since one of the groups is finite, we could have also shown directly why the copies of can be cancelled. Indeed, if is an isomorphism of abelian groups with finite, then the composition with the projection must annihilate the torsion group . Since the composite is surjective, it needs to be multiplication by on the component, so that is the kernel of this map. As this kernel also agrees with , restricts to an isomorphism , which is what we wanted to show.
Now that we have answered the question convering in Remark 5.6 of [14], let us comment on what we expect from the higher K-theory groups. Based on the computation of (where we showed that we can increase the rank of a matroid without changing its class), we believe that the K-theory of pointed matroids does not really differ much from that of pointed finite sets. More precisely:
Conjecture 4.16.
The map induced by the rank map and by the forgetful map to pointed finite sets is an equivalence of spectra. In particular, we have for all positive .
Based on Theorem 6.3 of [10] and on this article, this conjecture is currently known at the level of homotopy groups in degrees and .
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