On the homology of the commutator subgroup of the pure braid group
Andrea Bianchi

TL;DR
This paper investigates the homology of the commutator subgroup of the pure braid group, revealing infinite rank in certain homology groups and determining its cohomological dimension.
Contribution
It provides new insights into the homological structure of the commutator subgroup of pure braid groups, including explicit calculations of homology and cohomological dimension.
Findings
Homology groups contain free abelian groups of infinite rank for specified degrees.
Cohomological dimension of the commutator subgroup is exactly n-2 for n ≥ 2.
Homological properties are explicitly characterized for all n ≥ 2.
Abstract
We study the homology of , the commutator subgroup of the pure braid group on strands, and show that contains a free abelian group of infinite rank for all . As a consequence we determine the cohomological dimension of : for we have .
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On the homology of the commutator subgroup of the pure braid group
Andrea Bianchi
Mathematics Institute, University of Bonn, Endenicher Allee 60, Bonn, Germany
Abstract.
We study the homology of , the commutator subgroup of the pure braid group on strands, and show that contains a free abelian group of infinite rank for all . As a consequence we determine the cohomological dimension of : for we have .
Key words and phrases:
Pure braid group, commutator subgroup, cohomological dimension.
2010 Mathematics Subject Classification:
20F36, 55R20, 55R35, 55R80, 16S34, 20C07.
This work was supported by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany’s Excellence Strategy (EXC-2047/1, 390685813).
1. Introduction
Let and denote by the ordered configuration space of points in the complex plane:
[TABLE]
The pure braid group on strands is defined as .
In [3] David Recio-Mitter and the author posed the question of determining the cohomological dimension of , the commutator subgroup of the pure braid group, and conjectured that, for ,
[TABLE]
In this work we prove this conjecture by computing a large part of the homology of ; in particular we prove that contains a free abelian group of infinite rank in all degrees (see Theorem 6.1, Corollary 6.2 and Theorem 7.1).
To the best of the author’s knowledge there is no result in the literature concerning the homology of for large values of ; on the contrary the homology of the commutator subgroup of Artin’s full braid group [2] has been extensively studied [12, 17, 6, 4], as well as the homology of Milnor fibers of discriminant fibrations associated with other hyperplane arrangements in [7, 8, 5, 19].
Our strategy is the following. We consider the Salvetti complex associated with the -th braid arrangement: the cell complex is a classifying space for , and it has a covering which is a classifying space for . The group acts on by deck transformations, and the action is cellular: hence the associated cellular chain complex is a chain complex of modules over the commutative ring , and consequently the homology is also a -module.
We replace with a homotopy equivalent subcomplex ; the chain complex is only invariant for the action of a certain subgroup , and we restrict this action also in homology, i.e. we consider as a module over the commutative ring .
We define a filtration on ; the associated Leray spectral sequence, after localisation to the quotient field of , collapses on its first page: more precisely we have for all . This proves the statement for (see Theorem 6.1).
To prove the statement in lower degrees we consider the interaction between commutator subgroups of different pure braid groups (see Theorem 7.1).
2. Preliminaries
We recall some classical constructions and results about configuration spaces and pure braid groups.
For all there is a map , which forgets the th point of each configuration. This is a fiber bundle with fiber the punctured plane , called the Fadell-Neuwirth fibration (see [10]):
[TABLE]
The space is a classifying space for the free group on generators , in particular it is an aspherical space. An induction argument shows that is also aspherical, and therefore is a classifying space for its fundamental group . We obtain a short exact sequence
[TABLE]
Definition 2.1**.**
For all there is a forgetful map , which forgets all points of a configuration except the -th and the -th. This map of spaces induces a map, that we still call , on fundamental groups:
[TABLE]
The collection of all these maps gives a homomorphism of groups .
A classical result by Arnold [1] states that is the abelianisation homomorphism, i.e. along the map induced by . In this article we focus on the group , the commutator subgroup of the pure braid group.
3. Two classifying spaces for
We introduce two convenient models for the classifying space of .
Definition 3.1**.**
We define the space . A point in is determined by a configuration together with a choice of a logarithm of , for all :
[TABLE]
This space has a topology as subspace of .
There is a covering map , which forgets the numbers . The fiber is isomorphic to : to see this fix a point lying over some point . Let be any other point lying over : then there are integers such that for all . Viceversa given integers one can define a point in the fiber of by setting for all .
The last construction gives a free action of on ; this is an action by deck transformations of and is transitive on fibers of : therefore is the whole group of deck transformations of and there is a short exact sequence
[TABLE]
We can then conclude that , because is contained in the kernel of any map from to an abelian group.
On the other hand the maps lift to maps : the map is defined by forgetting all data except and .
The space is contractible: this is a particular case of Lemma 3.7, and can be checked also directly. Therefore is a subgroup of contained in the kernel of all maps , i.e. . We obtain the following lemma.
Lemma 3.2**.**
The space is a classifying space for the group .
The action of on induces an action of the ring on , so our first attempt is to study as a module over this ring.
Definition 3.3**.**
Let be the ring of Laurent polynomials in variables . The variable corresponds to the generator of which is dual to the map , i.e. for all and we have .
The ring is a domain and we call its quotient field.
The following lemma tells us that cannot be too large.
Lemma 3.4**.**
[TABLE]
Proof.
Consider the following homotopy of the space into itself. At time [math], the map is the identity of ; at time we rotate each configuration by an angle counterclockwise, adjusting logarithms:
[TABLE]
At time , the map preserves all ’s and shifts all ’s by : this last map is precisely the map
[TABLE]
i.e. the product of all deck transformations .
Since is homotopic to the identity of , it induces the identity map on .
Hence , as a -module, is -torsion, in particular its -localisation vanishes. ∎
The proof of the previous lemma tells us that the variable acts on as the product ; therefore it seems convenient to replace with a smaller ring, containing one variable less.
Definition 3.5**.**
We call
[TABLE]
the ring of Laurent polynomials in variables. is naturally a subring of by identifying each with the corresponding , and therefore each -module is also a -module.
We can also identify as the quotient of by the ideal generated by the element . The composition of maps of rings is the identity of .
The ring is a domain, and we call its quotient field.
We want now to study as a -module. We introduce our second model of a classifying space for .
Definition 3.6**.**
The space is defined as the subspace of of configurations such that , and .
The space is not invariant under the action of the whole group on : the action of consists in shifting by , and this is not allowed inside . The other generators of preserve ; we conclude that has a natural structure of module, and the inclusion map induces a map of -modules in homology.
Lemma 3.7**.**
* is a deformation retract of , and therefore it is also a classifying space for .*
Proof.
We define a homotopy starting with the identity of and ending with a retraction onto ; the space will be fixed pointwise throughout the homotopy.
Let . Then
[TABLE]
∎
4. Chain complexes
In this section let be fixed. Our next aim is to describe explicitly a chain complex that computes the homology of . We first recall the classical chain complex computing the homology of : it can be seen both as the dual of the reduced cochain complex of the one-point-compactification of , in the spirit of Fuchs [13], or as chain complex associated with the Salvetti complex [18] of the -th braid arrangement.
Definition 4.1**.**
An ordered partition of of degree is a partition of into non-empty subsets , where each piece is endowed with a total order.
For we write if precedes in the order associated with , and we keep writing if is smaller than as natural numbers.
We define the chain complex . Let be the free abelian group with one generator (also called cell) for each ordered partition of of degree .
In order to describe the boundary maps of it is enough, for any two ordered partitions and of degree and respectively, to give a formula for the boundary index , i.e. the coefficient of in . There are two possibilities:
- •
is obtained from by
- –
splitting some piece into two pieces and , each having as total order the restriction of the total order on ;
- –
setting for and for , with the same total orders.
Then
[TABLE]
where, for an ordered set and a subset , we define as the parity of the number of couples of elements of with , and .
- •
is not obtained from as before. Then .
The chain complex is the cellular chain complex of the Salvetti complex : it is a finite cell complex contained in , onto which deformation retracts [18].
Alternatively, in the spirit of Fuchs [13], one can consider the following stratification of . For every ordered partition of some degree , we consider the subspace consisting of all configurations satisfying the following properties:
- •
there are exactly vertical lines in passing through some of the points;
- •
for , the -th vertical line from left contains precisely the points with , and these points are assembled from the top to the bottom according to the total order .
In particular for configurations the following properites hold:
- •
for all , if and with , the point lies on left of the point , i.e. ;
- •
for all , if both and belong to the same piece and if , then lies above , or equivalently .
The one-point compactification of has a CW structure given by the subspaces together with the point at infinity . The associated reduced cellular cochain complex is precisely the one described in Definition 4.1. Note that each cell is modeled on the interior of a product of simplices
[TABLE]
The local coordinates are the horizontal positions of the vertical lines and the vertical positions of the points on these lines. We regard as a manifold of dimension ; an orientation can be given by declaring a total order on the simplicial local coordinates, and we choose the lexicographic order associated with the product structure written above.
With this convention, the boundary index in the reduced cellular chain complex of equals the formula for in Definition 4.1.
The space is a -dimensional manifold and its stratification by the subspaces gives rise to a Poincaré-dual cell complex, which is exactly the Salvetti complex .
The space has a covering corresponding to the subgroup of its fundamental group , and we can lift to the cell complex structure on . The group of deck transformations acts freely on the cells of ; the associated chain complex is a chain complex of finitely generated, free -modules.
Definition 4.2**.**
We define a chain complex . Let be the free abelian group with one generator (called cell) for each choice of the following set of data:
- •
an ordered partition of of degree ;
- •
integers for all .
The boundary map has a similar formula as in Definition 4.1. Consider cells and in degrees and respectively.
- •
Suppose that the ordered partition is obtained from as in the first case in Definition 4.1, splitting some into and . Suppose that for all satisfying
- –
;
- –
in ;
- –
and
we have . Finally, suppose that for all other couples of indices we have . Then
[TABLE]
- •
If cannot be obtained from as before, then the boundary index is zero.
Similarly as before, we can stratify as follows: for all as in Definition 4.2, consider the subspace of determined by the following properties:
- •
is a connected component of , where is the usual covering map;
- •
for all , there exists a configuration , depending on and , such that one of the following four situations occurs, depending on the position of and in the ordered partition :
- –
and , assuming and for some ;
- –
and , assuming for some , and ;
- –
and , assuming and for some ;
- –
and , assuming for some , and .
This stratification is the pull-back along of the stratification on . We can add a point to and obtain a space with a CW structure with the cells together with the point .
The space is not the one-point compactification of , but it is universal among topological spaces satisfying the following properties:
- •
is obtained from by adding one point ;
- •
for every meeting finitely many strata , the closure of in is compact.
The genuine one-point compactification of would have a coarser topology than , and in particular it would not have the topology of a CW complex.
The chain complex coincides with the complex of reduced, compactly supported cochains of ; the formulas for the indices are the same because we lift the canonical orientations of cells to their preimages along . The manifold is stratified by the spaces and there is a Poincaré dual cell complex, which is precisely the covering of the Salvetti complex .
Putting together all -summands generated by cells for fixed and varying we obtain one -summand of : the action of on this summand is analogous to the one discussed for the space (see the discussion preceding Lemma 3.2): multiplication times consists in shifting the number by 1, while keeping the other numbers as well as the ordered partition .
We note that is a chain complex of finitely generated, free -modules; a -basis is given by those elements with for all ; we call these basis elements to distinguish them from the elements generating over .
The differentials of with respect to the basis of the elements are expressed in a similar way as in Definition 4.2, but boundary indices are no longer always equal to [math] or , rather they can take the form of a product of some variables , with a sign determined in the same way as in Definition 4.2. It is however still true that all boundary indices of are either [math] or invertible elements of .
There is a natural map of chain complexes of abelian groups, mapping the generator to the generator : this map is induced by the covering map , which by construction is a cellular map.
Definition 4.3**.**
The chain complex contains a subcomplex of free abelian groups generated by cells such that:
- •
there are indices with and ;
- •
.
Note that is a subcomplex of abelian groups, and in particular is closed along boundary maps: if is a generator of , then and already belong to different pieces of the partition , so that cannot change along boundaries, according to Definition 4.2. The degrees of cells in range from [math] to , because there are always at least two pieces in the partition.
Lemma 4.4**.**
The chain complex computes the homology of .
Proof.
The space can be also defined as follows. Let be the subspace of of configurations with and . The space is the ordered configuration space of points in the -punctured plane, so it is the fiber over of the bundle map forgetting all points but the first two (see Definition 2.1).
The space is aspherical, and its fundamental group is the kernel of the map induced by on fundamental groups; moreover , where the isomorphism is exhibited by the collection of maps with .
The commutator subgroup of can be identified with
, and is the covering of corresponding to this group.
The space is the complement in of a hyperplane arrangement: using as coordinates of we are considering the following hyperplanes with real equations
- •
, for ;
- •
, for ;
- •
, for .
Hence also deformation retracts onto a Salvetti complex, that we call . Using the definition of the Salvetti complex [18] it is straightforward to check that the cellular chain complex of is isomorphic to the subcomplex of generated by cells satisfying the first condition of Definition 4.3.
Another possibility is the following. For every ordered partition satisfying the first condition of Definition 4.3, we can consider the subspace
[TABLE]
containing configurations such that the point belongs to the subspace . The subspaces , together with the point at infinity , give a CW structure of the one-point compactification of the manifold . The reduced cellular cochain complex of the space is by construction isomorphic to the subcomplex of generated by cells satisfying the first condition of Definition 4.3, up to a shift in dimension due to the fact that has (real) dimension , whereas has dimension . The Salvetti complex is the Poincaré dual of the cell decomposition of , and its cellular chain complex is also isomorphic to .
We can now restrict the covering first to a connected covering , and then to a connected covering . Note that is only one connected component of : there is indeed one connected component for any fixed value of .
We pull back the cell structure on along to a cell structure on ; thus the chain complex associated with is precisely . ∎
We define filtrations on the chain complexes that we have introduced.
Definition 4.5**.**
For each generator of there is an index such that : we denote .
We filter in the following way: a generator in some degree has height , with , if there are exactly indices such that . Note that by Definition 4.1 the height can only decrease along boundaries in .
In the same way we can filter the chain complex : a generator has the same height as the corresponding generator of . Note that we obtain a -invariant filtration on : in other words becomes a filtered chain complex of -modules.
The chain complex has a natural action of the group ; as we have already seen, the group can be identified with the kernel of the map , and is generated by elements for with . Hence can be seen as a chain complex of free modules.
Definition 4.6**.**
We consider as a chain complex of free modules and call the basis containing those elements that lie in .
The chain complex inherits a filtration from , with heights ranging from [math] to : this is a filtration in modules.
We call the subcomplex generated by cells of height , and the th filtration stratum.
Note that is a filtered basis for .
5. Morse flows
In this section we simplify the complex to a chain complex with fewer generators: we use Forman’s discrete Morse theory, which was first introduced in [11]; see [14] or [15] for an introduction to discrete Morse theory. The Morse complex that we present has already appeared in a similar way in [9] and [16].
Definition 5.1**.**
Recall from Definition 4.6 that is a basis for as a chain complex of finitely generated, free -modules. For a cell , the index was introduced in Definition 4.5. We define a matching on :
- •
a cell is critical if (i.e. ), and if is the last element of according to (i.e. for all with );
- •
a cell is collapsible if is not the last element of . In this case the redundant partner of is , where is obtained from by splitting into and , as in Definition 4.2 with , and is restricted to the two pieces. Informally, we push all elements lying below to the left. Note that . We write , meaning that the couple is in .
- •
a cell is redundant if and is the last element of according to . In this case the collapsible partner of is , where is obtained from by concatenating and into : on the new set the order is defined by extending on and with the rule for all and . In particular for all . Informally, we push the column on left of 1 underneath 1. We write .
By Definition 4.2 if two cells are matched, then is invertible in .
To check that is acyclic, note first that is compatible with the filtration of the chain complex , hence it suffices to check that is acyclic on each filtration stratum .
Let be an alternating path of three distinct cells of degrees , all having the same height . This means that the redundant cell is matched with the collapsible cell , and that . Suppose also that is redundant.
Then both and are obtained from by splitting precisely the piece as in Definition 4.2: indeed is not the last element in , but is the last element of both and .
Moreover there are exactly two ways to split in two pieces, so that the following conditions hold:
- •
becomes the last element of its piece;
- •
the height doesn’t decrease, i.e. all elements preceding in still belong to the same piece as and precede .
The two pieces must be, in some order, and , and we can only choose which piece is split to the left and which to the right.
If is split to the left, then we get the redundant partner of , that is, ; in the other case we must get .
We conclude that , and ; in particular . This shows that the matching is acyclic on each stratum , because the index strictly increases along alternating paths.
Definition 5.2**.**
We call the Morse complex associated with the acyclic matching : it is a chain complex of finitely generated, free -modules, with basis given by -critical cells in . The chain complex is also a filtered chain complex of -modules: the subcomplex is generated by -critical cells of height , and the -th filtration stratum is denoted by .
We conclude this section by analysing more carefully the structure of the filtration strata.
Definition 5.3**.**
Let be a subset of containing . We denote by the ring . This is a domain and is naturally contained in ; its quotient field is denoted by , and there is an inclusion . In the particular case we have .
Let and be defined in analogy with Definitions 4.1 and 4.2 but using, instead of the set of indices , its subset . In particular generators of are given by ordered partitions of ; generators of are given by an ordered partition of together with a choice of integers for all with .
Note that is a chain complex of finitely generated, free -modules, supported in degrees ranging from [math] to . In the particular case we have that consists of a copy of in degree 0.
Lemma 5.4**.**
Let ; then there is an isomorphism of chain complexes of -modules
[TABLE]
where the sum is taken over all sets with and . This isomorphism shifts degrees by .
Proof.
Recall that the differential in the chain complex is defined as follows: for two -critical cells and in the boundary index is the sum of the weights of all alternating paths from to .
If and have the same height , then an alternating path must contain only cells of height . Since is critical, is the last element of , and splitting in two pieces would let the height of decrease to a smaller height in : hence is obtained from by splitting some other piece with , and therefore is already critical, hence .
Thus the differential in the chain complex is isomorphic to the differential obtained from Definition 4.2 by allowing only a splitting in two pieces of some piece of the partition with .
In particular we can split our chain complex into many subcomplexes according to which elements, all different from , appear in and in which order , provided that is the last element of .
To determine one of these subcomplexes we can equivalently choose a set of elements, with , and declare that the other elements , including 1, are the elements of . Moreover there are exactly ways to order these elements inside , if we require to be the last in the order: each of these possible choices of on gives rise to a different subcomplex.
Finally we note that each of these subcomplexes is isomorphic to the chain complex , where the isomorphism is given by mapping the -critical cell to the cell : this map has degree . ∎
6. The spectral sequence with coefficients in
In this section we prove that . More precisely we prove the following theorem.
Theorem 6.1**.**
For the graded -vector space
[TABLE]
has dimension in degree and vanishes in all other degrees.
This means, in particular, that contains an embedded copy of , which for is a free abelian group of infinite rank.
The following is an immediate consequence of Theorem 6.1.
Corollary 6.2**.**
For the cohomological dimension of is .
Proof.
We have because . Moreover, as already seen in the proof of Lemma 4.4, the space deformation retracts onto the space , which is a cell complex of dimension ; hence . ∎
Proof of Theorem 6.1.
We consider the filtered chain complex . Since localisation is exact we can compute as the homology of the chain complex , which is a filtered chain complex of -vector spaces.
The first page of the associated Leray spectral sequence is
[TABLE]
and our aim is to show that the latter groups are all trivial, except for and , where we have
[TABLE]
Once this statement is proved, Theorem 6.1 follows immediately because the spectral sequence collapses on its first page.
By Lemma 5.4 the chain complex is isomorphic to the chain complex . Since the ring is just , and since the chain complex is just a copy of in degree [math], we have that the filtration stratum is concentrated in degree and its homology is , also concentrated in degree .
Tensoring with we have that , and for all .
We want now to show that the chain complex is acyclic for all . By Lemma 5.4 it suffices to prove that, for any set containing , the chain complex
[TABLE]
is acyclic. We note that contains , so we can equally consider
[TABLE]
and the latter is acyclic because is acyclic by Lemma 3.4, and extending the field is exact. ∎
We note that it was not necessary to localise with respect to all non-zero elements, i.e. passing from to its quotient field .
Definition 6.3**.**
Let be a finite subset of containing . We call
[TABLE]
Define also
[TABLE]
where the product is extended over all subsets containing .
Then the same argument of the proof of Lemma 3.4 tells us that, for all subsets with , we have
[TABLE]
Therefore we can repeat the proof of Theorem 6.1 to show that
[TABLE]
is concentrated in degree , where it is equal to .
7. Homology in lower degrees
In this section we prove non-triviality of in all degrees . More precisely, we prove the following theorem.
Theorem 7.1**.**
For all the group contains a free abelian group of infinite rank.
Proof.
By Theorem 6.1 we know that contains a free abelian group of infinite rank. In the following we fix and prove that has the same property.
Consider the map that forgets the last points of a configuration (compare with the maps from Definition 2.1):
[TABLE]
The map is a fibration (see [10]) and there is a section given by adjoining points far on the right: formally we set and then we define
[TABLE]
We have induced maps on fundamental groups and ; the composition is the identity of .
The maps and restrict to maps between commutator subgroups; in particular the composition is the identity of .
This implies that the induced map in homology
[TABLE]
is injective, and again by Theorem 6.1 we know that contains a free abelian group of infinite rank. ∎
8. Future directions
Computing the homology of as a -module seems a difficult task, in particular because is not a principal ideal domain and we lack a good classification of finitely generated modules over . We only observe that is finitely generated over : indeed the chain complex is finitely generated over , and is a noetherian ring.
Computing directly as an abelian group seems not to be easy either. In Theorems 6.1 and 7.1 we have proved that contains a free abelian group of infinite rank for ; we conjecture that is indeed a free abelian group, and in particular is torsion-free. Our conjecture is related to a conjecture by Denham [8] on the structure of the homology of the Milnor fibre of a complexified real arrangement; this conjecture was investigated also by Settepanella [19]. Note that for our conjecture holds, as is a free group.
Finally, it would also be interesting to study as a representation. Denote by Artin’s braid group on strands [2], and by the -th symmetric group. There is a short exact sequence
[TABLE]
In particular is a normal subgroup of ; since is a characteristic subgroup of , is also normal in and we have a short exact sequence
[TABLE]
It would be interesting to understand as a representation of
.
Acknowledgments
The author would like to thank Carl-Friedrich Bödigheimer, Filippo Callegaro, Florian Kranhold, Mark Grant, Davide Lofano, Martin Palmer, Giovanni Paolini, Oscar Randal-Williams, David Recio-Mitter and Mario Salvetti for useful discussions and precious comments during the preparation of this paper.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] Vladimir I. Arnold. The cohomology ring of colored braids. Matematicheskie Zametki , 2:227–231, 1969.
- 2[2] Emil Artin. Theorie der Zöpfe. Abhandlungen aus dem Mathematischen Seminar der Universität Hamburg , 4:47–72, 1925.
- 3[3] Andrea Bianchi and David Recio-Mitter. Topological complexity of unordered configuration spaces of surfaces. Algebraic and Geometric Topology , 19:1359–1384, 2019.
- 4[4] Filippo Callegaro. The homology of the Milnor fiber for classical braid groups. Algebraic and Geometric Topology , 6:1903–1923, 2006.
- 5[5] Filippo Callegaro, Davide Moroni, and Mario Salvetti. Cohomology of affine Artin groups and applications. Transactions of the American Mathematical Society , 360(8):4169–4188, 2008.
- 6[6] Corrado De Concini, Claudio Procesi, and Mario Salvetti. Arithmetic properties of the cohomology of braid groups. Topology , 40:739–751, 2001.
- 7[7] Corrado De Concini, Claudio Procesi, Mario Salvetti, and Fabio Stumbo. Arithmetic properties of the cohomology of Artin groups. Ann. Scuola Norm. Sup. Pisa Cl. Sci. (4) , XXVIII:695–717, 1999.
- 8[8] Graham Denham. The Orlik-Solomon complex and Milnor fibre homology. Topology and its Applications , 118:45–63, 2002.
