Deletion-restriction for sheaf homology of graded atomic lattices
Brent Everitt, Paul Turner

TL;DR
This paper develops a long exact sequence for sheaf homology on graded atomic lattices, enabling computation of hyperplane arrangement lattice homology and generalizing Lusztig's classical result.
Contribution
It introduces a deletion-restriction long exact sequence for sheaf homology on graded atomic lattices, extending previous work to new classes of arrangements.
Findings
Derived a long exact sequence relating homology of lattices and their deletions/restrictions.
Computed the sheaf homology of hyperplane arrangement lattices using the new sequence.
Generalized Lusztig's classical result to a broader context.
Abstract
We give a long exact sequence for the homology of a graded atomic lattice equipped with a sheaf of modules, in terms of the deleted and restricted lattices. This is then used to compute the homology of the arrangement lattice of a hyperplane arrangement equipped with the natural sheaf. This generalises an old result of Lusztig.
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
11institutetext: Brent Everitt: Department of Mathematics, University of York, York YO10 5DD, United Kingdom. 11email: [email protected]. Paul Turner: Section de mathématiques, Université de Genève, 2-4 rue du Lièvre, CH-1211, Geneva, Switzerland. 11email: [email protected].
Deletion-restriction for sheaf homology of graded atomic
lattices
Brent Everitt and Paul Turner The second author was partially supported by NCCR SwissMAP
Abstract
We give a long exact sequence for the homology of a graded atomic lattice equipped with a sheaf of modules, in terms of the deleted and restricted lattices. This is then used to compute the homology of the arrangement lattice of a hyperplane arrangement equipped with the natural sheaf. This generalises an old result of Lusztig.
††dedicatory: Dedicated to Marcia Everitt (1932-2018) and Ken Turner (1927-2014)
Introduction
This paper is about graded atomic lattices, equipped with sheaves of modules, and their homology. Important examples in nature are the face lattices of polytopes, the intersection lattices of hyperplane arrangements, and the lattices of flats of matroids. This last family comprises precisely the geometric lattices. When studying lattices a key role is played by deletion-restriction, where the lattice may be decomposed into two pieces with respect to some atom : the deletion and the restriction . For example, the characteristic polynomial of a geometric lattice may be expressed in terms of the characteristic polynomials of the deletion and restriction.
When is equipped with constant coefficients – that is, the sheaf is the constant sheaf – then the homology reduces to the ordinary simplicial homology of the order complex of , and one can avail oneself of standard topological tools. For example, an argument using a Mayer-Vietoris sequence is enough to fully compute the homology of a geometric lattice Folkman66; Bjorner82. The long exact sequence used in the calculation is another manifestation of deletion-restriction, relating the homology of with that of and ; see Orlik-Terao92*§4.5 for details.
If the sheaf is non-constant then the topology of can play a relatively minor role in homology – the space can be contractible for example, but the sheaf homology may be highly non-trivial. This makes the calculation of homology for arbitrary sheaves less straightforward, and the techniques used for constant coefficients do not simply generalise.
Nevertheless, for an arbitrary sheaf it turns out there is a deletion-restriction long exact sequence, and this is the first main result of the paper:
**Main Theorem. **
Let be a graded atomic lattice equipped with a sheaf . Then for any atom there is a long exact sequence
[TABLE]
where is the map induced by the , for , and the universality of the colimit.
Each lattice has had its minimum element removed, a necessary requirement for a lattice when considering its sheaf homology. If minima are not removed then, for general reasons, the homology will be concentrated in degree zero. When the coefficients are constant, both the minimum and the maximum have to be removed to avoid the homology completely collapsing. When the sheaf is non-constant there is no a priori reason to remove the maximum. We also warn the reader that at the generality of graded atomic lattices , the restriction is not itself atomic. To make inductive arguments therefore, one must start with an carrying more structure: for example the face lattice of a polytope or a geometric lattice – see §§1.1-1.2.
In the case of a linear hyperplane arrangement, the associated arrangement lattice has elements the intersections of hyperplanes. As these intersections are again linear spaces this gives rise to a canonical sheaf on the lattice of intersections. We refer to this as the natural sheaf. Our main application of the deletion-restriction long exact sequence gives a complete calculation of the reduced homology in this case:
**Main Application. **
Let be the intersection lattice of a hyperplane arrangement with and let be the natural sheaf on . Then is trivial when and
[TABLE]
where is the characteristic polynomial of .
The quantity appearing on the right-hand side is known (in the more general context of matroids) as the beta-invariant (see MR921071*§7.3). We note that Yuzvinsky Yuzvinsky91 formulated the notion of a local sheaf to generate similar vanishing homology results, but these ideas are not readily applicable to the situation above.
Our original motivation was a result of Lusztig Lusztig74*Theorem 1.12, where he proved that if is a space over a finite field, is the hyperplane arrangement consisting of all the hyperplanes in , and is the natural sheaf, then vanishes in degrees . Lusztig’s interest in natural sheaves on arrangement lattices arose in his study of the discrete series representations of for a finite field. As a corollary to our main application we extend Lusztig’s result to any arrangement:
**Corollary. **
Let be the intersection lattice of a hyperplane arrangement in the vector space and let . Suppose that and let be the natural sheaf on . Then vanishes in degrees with and
[TABLE]
where is the Möbius function of .
We note that while our calculations involving hyperplane arrangements have homology vanishing in all but top degree, this behaviour is the exception rather than the rule. One can readily find lattices and sheaves whose homology is highly non-trivial. One example is the the Khovanov homology of a link diagram Khovanov00 which may be interpreted in terms of sheaf homology (see EverittTurner15; EverittTurner14). In this case there are many non-vanishing intermediate degrees, despite the underlying lattice being contractible. Even when the sheaf structure maps are all injections one easily finds non-trivial homology in intermediate degrees. A natural example is in the context of “sheaves on buildings”. Indeed, Lusztig’s result can be viewed as the case of the building of equipped with the fixed point sheaf of the natural representation, for which the structure maps are all inclusions. There are similar situations – the building of for example – where the homology is non-vanishing in some intermediate degrees (see Ronan_Smith85).
The paper is organised as follows. In Section 1 we set down the basics on lattices, and in particular discuss the notion of a dependent atom, that will play a key role in inductive arguments. In Section 2 we remind the reader about the basics of sheaf homology on posets – both unreduced and reduced. We also present the Leray-Serre spectral sequence arising from a poset map, which plays a key role. In Section 3 we present a deletion-restriction long exact sequence for arbitrary sheaves (Theorem 3.1) and also give a version using reduced homology (Corollary 3). In Section 4 we calculate, as an application, the sheaf homology of a hyperplane arrangement equipped with the natural sheaf (Theorem 4.1) and put this in a form which makes direct comparison to Lusztig’s result (Theorem 4.3). We end with a few remarks about the reduced broken circuit complex, whose homology also features the beta-invariant.
We are grateful to the referee for pointing out to us the literature concerning broken circuits and the beta-invariant.
1 Lattices
In §§1.1-1.2 we recall basic facts about posets, lattices, geometric lattices and arrangement lattices. Standard references for this material are Birkhoff79; Stanley12; MR2383131; Orlik-Terao92. In §1.3 we set down facts about dependent atoms from Everitt-Fountain13 that will be useful in the inductive arguments of §4.
1.1 Basics
Let be a finite poset. If and for any we have either or , then is said to cover , and we write . is graded if there exists a function such that (i) implies , and (ii) implies . A minimum is an element such that for all and a maximum is an element such that for all . If has a minimum , then the standard grading on is defined by taking to be the supremum of the lengths of all poset chains from to . All the posets in this paper will be graded with the standard grading. The elements covering – those of rank – are called atoms. A poset map is a set map such that if .
A subset is upper convex if and implies that . If , the interval consists of those such that ; if the interval consists of those such that ; one defines , and similarly.
A lattice is a poset such that any two elements and have a unique supremum (or join) and a unique infimum (or meet) . A finite lattice has minimum equal to the meet of all its elements and maximum equal to the join of all its elements. A graded lattice is atomic if every element can be expressed – not necessarily uniquely – as a join of atoms, and with the empty join taken to be . The rank, , of a graded lattice is .
Examples of graded atomic lattices abound:
- •
If is a (finite) set then the free, or Boolean, lattice has elements the subsets of ordered by inclusion. It is a graded atomic lattice with , , join , meet , minimum , maximum and atoms the singletons – which we identify with . Any element has a unique expression as a join of atoms.
- •
A (convex) polytope in a real vector space is the convex hull of a finite set of points – see Grunbaum03; Ziegler95. The face lattice has elements the faces of ordered by reverse inclusion. This is a graded a atomic lattice (graded by ) with atoms the faces, join , meet the smallest face containing and , minimum and maximum (hence ).
- •
The partition lattice on the set consists of all partitions of ordered by refinement: if each is contained in some . The result is a graded lattice with ; , minimum the partition with all blocks singletons, maximum , and atoms the partitions with just one block not having size one.
- •
The intersections of a collection of hyperplanes ordered by reverse inclusion gives an arrangement lattice – see §1.2.
If is graded atomic with atoms , then for , define the deletion lattice to be the elements of that can be expressed as a join of the elements of (with the empty join taken to be ), and the restriction lattice to be the interval . The deletion is graded atomic with atoms , minimum , maximum and rank function . The restriction is graded but not in general atomic; if however is the face lattice of a polytope Ziegler95*Theorem 2.7 or an arrangement lattice (which includes the Boolean and partition examples) then is atomic.
We finish our review of the basics with an important object in the theory of enumeration. If is a field, then the Möbius function of is the -valued function on the intervals defined by
[TABLE]
and for all .
1.2 Geometric and arrangement lattices
A graded atomic lattice is geometric if the rank function satisfies
[TABLE]
for all and . The Boolean, partition and arrangement lattices above are geometric; the face lattices of polytopes are usually not. If is geometric then for a given atom , both and are again geometric lattices. The restriction has atoms , minimum , maximum and rank function .
Our main supply of geometric lattices will come from (linear) hyperplane arrangements. Let be a finite dimensional vector space over a field ; then an arrangement in is a finite set of linear hyperplanes in . The arrangement lattice has elements all possible intersections of hyperplanes in – with the empty intersection taken to be – and is ordered by reverse inclusion. Then is a geometric lattice with atoms the hyperplanes , and
[TABLE]
Given , the deletion lattice is the arrangement lattice , and similarly the restriction lattice is the arrangement lattice .
Some examples:
- •
Let be a basis for with corresponding coordinate functions . The coordinate arrangement consists of the hyperplanes having equations , for . The arrangement lattice is isomorphic to the Boolean lattice via the map .
- •
The symmetric group acts on by permuting basis vectors: for . This realises as a reflection group where the reflecting hyperplanes are those with equations for all . Collectively they form the braid arrangement – so called, when , as the space has fundamental group the (pure) braid group on strands. The arrangement lattice is isomorphic to the partition lattice via the map induced by maps to the partition with just one block not having size one.
- •
More generally, if is any finite reflection group, then the reflecting hyperplanes of form a reflectional arrangement.
When or , the only possibility for is that it be Boolean of rank . The arrangement lattices with 3 or fewer hyperplanes are shown in Figure 1. The first three are Boolean and the last is the partition lattice of a 3-element set. An arrangement lattice of rank 2 has the form shown in Figure 2.
An arrangement in the space is essential when , or equivalently, is the zero space. The characteristic polynomial of the arrangement is defined by
[TABLE]
where is the value of the Möbius function of the associated arrangement lattice on the interval , i.e. .
1.3 Dependence
There is a notion of independence in a lattice that mimics linear algebra. Let be a graded atomic lattice with atoms and write for the join of the elements in a subset . A set of atoms is independent if for all proper subsets of , and dependent otherwise. An atom in a dependent set of atoms with the property that is called a dependent atom. It is easy to show Everitt-Fountain13*§1.1 that if is dependent then there is an independent with , and that any subset of an independent set is independent.
Proposition 1
Let be a graded atomic lattice with independent atoms . Then is isomorphic to the Boolean lattice .
Birkhoff (Birkhoff79, IV.4, Theorem 5) proves this for a geometric lattice.
Proof.
In any element has a unique expression as a join of atoms. Since and share the same set of atoms and each element in may be written as a join of atoms, there is a canonical surjection given by
[TABLE]
We show that is injective and that is a poset map, hence is an isomorphism. Both follow from the following claim: if and , are any expressions as joins of atoms, then if and only if . To prove the “only if”’ part of the claim, let and suppose that for some . Then
[TABLE]
and after removing redundancies on the left (as joins commute and for all ) the right hand join of atoms is a proper subset of the left hand join of atoms. Taking the join of both sides with those atoms that are not any of the or gives on the left and on the right, for some a proper subset of . This contradicts the independence of . The “if” part of the claim is obvious.
Now let and be subsets of atoms with . Then by the claim we have and hence as is the identity map on . Thus, is injective. A similar argument shows that is a poset map. ∎∎
In a geometric lattice with atom set we have . Moreover, is independent if and only if , so the above shows that if and only if is Boolean.
Corollary 1
Let be a non-Boolean geometric lattice with hyperplanes. Then there exists a dependant atom such that
–
the deletion has atoms and ;
–
the restriction has at most atoms and .
2 Sheaf homology
In §§2.1-2.2 we recall the basics of sheaves on posets and the resulting homologies – standard references are Gabriel_Zisman67; Godement73; Quillen78; Quillen73. In §2.3 we recall a convenient tool for calculating homology: a Leray-Serre spectral sequence for which we reference Gabriel_Zisman67*Appendix II. In §2.4 we recall the notion of reduced homology.
2.1 Sheaves
Let be a commutative ring with . A sheaf111Strictly speaking we should say presheaf rather than sheaf, but as our posets are discrete (if one wishes to view them as topological objects) there is essentially no difference between presheaves and sheaves. on a poset is a contravariant functor
[TABLE]
to the category of -modules, where is interpreted as a category in the usual way. The category of sheaves on has objects the sheaves and morphisms the natural transformations of functors . We write for the homomorphism, or structure map, of the sheaf given by . Two important examples of sheaves are:
- •
For the constant sheaf is defined by for every and for every in .
- •
If is the intersection lattice of a hyperplane arrangement , then the natural sheaf on has just the space itself, and for in , the structure map is the inclusion of spaces .
If is a map of posets and is a sheaf on , then there is an induced sheaf on given by .
2.2 Homology
For any sheaf on the colimit is constructed by taking the quotient of by the submodule generated by all elements of the form where and . Taking colimits is right but not left exact, which earns them the privilege of left derived functors. These are called higher colimits and are denoted
[TABLE]
If is a short exact sequence of sheaves then there is a long exact sequence of modules:
[TABLE]
The homology of with coefficients in the sheaf are the higher colimits evaluated at the sheaf .
Homology can be computed using an explicit chain complex in the following way (details may be found in Gabriel_Zisman67*Appendix II). Recall that the order complex (or nerve) of the poset is the simplicial complex whose vertices are the elements of and whose -simplicies are the chains
[TABLE]
Let be the chain complex whose group of -chains is
[TABLE]
the direct sum over the -simplicies (3) of . If is an -simplex and , then will write for the element of that has value in the component indexed by and value [math] in all other components. The differential in is defined as follows. If
[TABLE]
for , then is given by
[TABLE]
The higher colimits may be computed as the homology of this complex:
[TABLE]
In the special case of the constant sheaf , the homology is just the ordinary simplicial homology of :
[TABLE]
If is a map of posets and is a sheaf on , then there is a chain map induced by . In particular, if is an inclusion, then is just the restriction of the sheaf to the subposet (in which case we will simply write for the restricted sheaf too) and is a subcomplex of .
There is a variation on the complex which uses only non-degenerate simplices. The group of -chains is
[TABLE]
where this time the sum is over non-degenerate simplices , and the differential is once again given by formula (4). Then, is a sub-complex of , and there is a homotopy equivalence . The following lemma gathers together some small results needed later.
Lemma 1
If is a finite graded poset, then only if . 2. 2.
If has a minimum or maximum, and is a constant sheaf, then and vanishes for . 3. 3.
If has a minimum , and is any sheaf, then and vanishes for . 4. 4.
If has a maximum , and is a sheaf on such that , then is isomorphic to .
Proof.
Part 1 follows immediately from the existence of ; part 2 follows from (5) and the fact that is contractible, as it is a cone on , where is the maximum or minimum. In the presence of a minimum the colimit functor is naturally isomorphic to the evaluation functor , which is exact, hence part 3. Finally, the complexes and are identical when , hence part 4. ∎∎
Remark:
If has a maximum but no minimum then, according to the Lemma, homology with constant coefficients still vanishes in every non-zero degree. However, this is far from the case when one allows more interesting sheaves . In general can be almost arbitrarily complicated.
2.3 The Leray-Serre spectral sequence
There is a spectral sequence for higher colimits given in Gabriel_Zisman67*Appendix II, Theorem 3.6; the following is the specialisation of this result from small categories to posets.
Let be a poset map and let be a sheaf on . For each define a sheaf on by
[TABLE]
where the sheaf denoted on the right is the restriction of to . If in then the structure map is induced by the inclusion .
Theorem 2.1 (Leray-Serre)
There is a spectral sequence
[TABLE]
We warn the reader that the sheaves in Gabriel_Zisman67*Appendix II are covariant, so the translation requires a number of headstands. The sequence is a special case of the results in MR0102537, where Grothendieck gives a spectral sequence that converges to the derived functors of a composite of two functors.
The following corollary is a homological version of the Quillen fibre lemma Quillen78, which states that if is a poset map such that for all , the fiber is contractible, then is a homotopy equivalence.
Corollary 2
Let be a surjective poset map, let be a sheaf on and let be the induced sheaf on . Suppose that for all the homology vanishes outside degree [math] and . Then there is an isomorphism
[TABLE]
Proof.
We have for and , with structure maps identified with . Thus and the spectral sequence of Theorem 2.1 collapses on the page with on the line. The result then follows. ∎∎
The conditions of the corollary occur most commonly in nature when for all the subposet has a minimum : for then by Lemma 1 part 3 the homology is concentrated in degree [math]. Moreover, by the surjectivity of , we have , hence .
2.4 Reduced homology for lattices
For the sheaf homology of a poset one needs to remove the minimum; otherwise – see Lemma 1, part 3. However there is a reduced version of homology which provides a way of remembering the minimum without rendering the homology almost trivial.
Let be a poset with minimum and let be a sheaf on . We can augment the chain complex by defining to be the sum of the structure maps over the . The reduced homology is the homology of this augmented complex . The map induces , which coincides with the map induced by the , using the universality of the colimit. We have
[TABLE]
and . One can also use the complex in all of the above.
3 The deletion-restriction long exact sequence
Given a graded atomic lattice equipped with a sheaf , then for an atom the deletion and restriction lattices and (as defined in §1.1) may be equipped with by restriction. The homology of these three lattices are tied together by a long exact sequence which we establish in this section. We remind the reader that at the generality of graded atomic lattices , the restriction is not itself atomic. To make inductive arguments, one must start with an carrying more structure: for example the face lattice of a polytope or a geometric lattice.
Theorem 3.1 (Deletion-Restriction Long Exact Sequence)
Let be a graded atomic lattice equipped with a sheaf . Then for any atom there is a long exact sequence
[TABLE]
where is the map induced by the , for , and the universality of the colimit.
In the proof of Theorem 3.1 will use the sub-poset of defined by . If is the set of atoms of , then for , let be those atoms and let . When we have . Define a mapping by
[TABLE]
Lemma 2
The map is a poset map and for any , the pre-image has minimum .
Proof.
Observe that for we have . Moreover, as , then for we have (if then trivially ). To show that is a poset map, suppose that in . It is easy to see that if are both in , or both not in , then . If and , then for some , hence . Finally, if and , then .
For the second claim, gives . If is an element of then , and in particular . If is itself in , then . If then so that . ∎∎
Proof.
(of the deletion-restriction long exact sequence). Equip with the restriction of . There is an inclusion of complexes
[TABLE]
with quotient where
[TABLE]
for is the sum over the non-degenerate simplices , and . The differential is given by
[TABLE]
and is the map for .
Notice that is a simplex in . There is an evident isomorphism between and the augmented complex , and in homology
[TABLE]
for . We also have and .
The short exact sequence
[TABLE]
thus induces a long exact sequence
[TABLE]
We finish the proof by showing that for all . For this we apply the Leray-Serre spectral sequence to the map of Lemma 2. The spectral sequence is of the form
[TABLE]
where for ,
[TABLE]
By Lemma 2, the poset has a minimum, so Lemma 1 part 3 then gives
[TABLE]
Therefore the spectral sequence has a single row () on which . The sequence thus collapses at the -page, and we conclude that .∎∎
We state as a corollary a special case that we will use on hyperplane arrangements in the next section.
Corollary 3 (Reduced Deletion-Restriction Long Exact Sequence)
Let be a graded atomic lattice equipped with a sheaf . Let be an atom such that is a surjection. Then, there is a long exact sequence
[TABLE]
Proof.
Consider the long exact sequence in the proof of Theorem 3.1, and let
[TABLE]
One can then show that . Now restrict to . One then gets that and so can be replaced by in the long exact sequence. Similarly maps onto , so we can also replace the last term in the sequence with its reduced version (the final is already [math] by the assumption in the Corollary). Then continue as in the proof of Theorem 3.1, replacing by . All the other terms in the sequence (*) are automatically equal to their reduced versions. ∎∎
4 Application to hyperplane arrangements
In this section is the intersection lattice of a hyperplane arrangement in the vector space , and is the natural sheaf on (see §2.1).
4.1 Reduced homology
Our goal is to compute , and our main tool is Corollary 3, the reduced deletion-restriction long exact sequence. To apply it we need the following small result.
Lemma 3
Let be the intersection lattice of a hyperplane arrangement with and let be the natural sheaf on . Then the map induced by the , for , is surjective.
Proof.
Since , the arrangement has at least two distinct hyperplanes, whose vector space sum is . The result follows immediately from the definition of colimit. ∎∎
For any atom in an arrangement lattice , the restriction is also an arrangement lattice with minimum ; in particular is graded atomic and is a surjection, so we can use the long exact sequence of Corollary 3 to make inductive arguments. Throughout this section we will therefore use reduced homology.
We begin with the special cases of rank 2 lattices and of Boolean lattices.
Proposition 2
Let be the intersection lattice of a hyperplane arrangement with and let be the natural sheaf on . Then is trivial when and
Proof.
The homology is concentrated in degrees 0 and 1. The complex of §2.2 can be written out explicitly, from which it is easily seen that is injective, hence . Moreover
[TABLE]
so that
[TABLE]
The augmentation is surjective by Lemma 3, so that
[TABLE]
∎
Proposition 3
Let be a Boolean lattice that is the intersection lattice of a hyperplane arrangement with , and let be the natural sheaf on . Then is trivial.
Proof.
We use induction on the number of hyperplanes, which in the Boolean case equals the rank .
The base case, , follows from Proposition 2, so suppose . For any hyperplane the deletion and restriction are again Boolean, and of rank . Thus and by induction. The result then follows from the reduced deletion-restriction long exact sequence. ∎∎
We now state and prove our main application:
Theorem 4.1
Let be the intersection lattice of a hyperplane arrangement with and let be the natural sheaf on . Then is trivial when and
[TABLE]
where is the characteristic polynomial of .
Proof.
If has rank and then the characteristic polynomial is
[TABLE]
and we easily calculate
[TABLE]
This, and Proposition 2, proves the theorem for rank 2 lattices.
If is Boolean of rank and , then the characteristic polynomial is
[TABLE]
The derivative of vanishes at , so this and Proposition 3 prove the theorem for Boolean lattices.
We now proceed by induction on the number of hyperplanes, and where . If then , so we take as our base case :
– The base case .
As , then §1.2 shows that the only possibility for is that it be Boolean of rank , and the theorem has already been proved in this case.
– The vanishing degrees when .
We may assume that is non-Boolean of rank and – though being non-Boolean is not part of the inductive hypothesis.
Corollary 1 guarantees that the non-Boolean has a dependent atom , so the deletion is an arrangement lattice with hyperplanes and . Thus, the inductive hypothesis, and hence the result, holds for .
Corollary 1 again gives the restriction is an arrangement lattice with at most hyperplanes and . If then the result holds for by Proposition 2. If then , and there must be at least 3 hyperplanes; the result then holds for by induction.
The reduced deletion-restriction long exact sequence
[TABLE]
then has trivial for and trivial for , or equivalently, for . Thus, for .
– The dimension in degree .
Let be an integer-valued function, defined on arrangement lattices of rank , that satisfies the following three properties:
- (1)
, if is a rank 2 lattice with atoms; 2. (2)
, if is Boolean; 3. (3)
, where is a dependent atom in .
If such a function exists it is unique: indeed by Corollary 1 we may continue to apply the recursive relation (3) until we find Boolean lattices – whose values are given by (2) – or rank 2 lattices, whose values are given by (1).
Let
[TABLE]
We claim that satisfies (1), (2) and (3) above. Courtesy of Proposition 2, we have when has rank – hence (1) – and Proposition 3 gives for Booleans, so (2) is also satisfied. The vanishing degrees above leaves only the short exact fragment:
[TABLE]
of the deletion-restriction long exact sequence. We immediately see that satisfies (3).
Now define
[TABLE]
We have already calculated at the beginning of the proof for rank two lattices and for Booleans, showing satisfies (1) and (2) above. Furthermore, the characteristic polynomial satisfies the relation:
[TABLE]
from which it follows that
[TABLE]
Differentiating and specialising to shows that also satisfies (3). By uniqueness we conclude that , giving the dimension in degree to be as claimed. ∎∎
4.2 Unreduced homology
It is easy to compute unreduced homology from the above. Reduced and unreduced only differ in degree zero where we have a short exact sequence
[TABLE]
We immediately get
Proposition 4
Let be the intersection lattice of a hyperplane arrangement with and let be the natural sheaf on . Then is trivial when or . Moreover,
–
If we have and the potentially non-trivial group in degree has the dimension given in Theorem 4.1.
–
If we have
4.3 Generalising a result of Lusztig
When using constant coefficients, the homology of a poset with a maximum is concentrated in degree zero for general reasons (see Lemma 1). To avoid this collapse the maximum is normally removed before taking homology. The same is true when the poset has a minimum. For a more general sheaf the presence of a maximum does not a priori concentrate the homology in this way. Nonetheless, for consistency it is tempting to remove the maximum in this case too, as in the following celebrated result of Lusztig Lusztig74*Theorem 1.12.
Theorem 4.2
(Lusztig)*
Let be a vector space over a finite field of dimension and let be the arrangement consisting of all the hyperplanes in . Let be the associated arrangement lattice and be the natural sheaf. Then vanishes in the degrees and .*
In this section we make explicit the connection between our Theorem 4.1 and Lusztig’s result. In particular we describe for any arrangement lattice equipped with the natural sheaf .
Recall §1.2 that an arrangement is essential when . In particular, for the natural sheaf on , we have , and so by Lemma 1 part 4 we get . As the arrangement in Lusztig’s result is essential, Theorem 4.2 follows immediately from Theorem 4.1 and Proposition 4. In fact we get more than is claimed in Theorem 4.2 as we give the dimension of the top degree homology as well.
We are also interested in non-essential hyperplane arrangements, where . The following recasts our Theorem 4.1 in a way that it can be directly seen as a generalisation of Lusztig’s result.
Theorem 4.3
Let be the intersection lattice of a hyperplane arrangement in the vector space and let . Suppose that and let be the natural sheaf on . Then vanishes in degrees with and
[TABLE]
Proof.
Define a new sheaf on by
[TABLE]
with obvious structure maps induced from . As is essential, Lemma 1 part 4 gives
[TABLE]
To prove the result we must therefore compute . There is a short exact sequence of sheaves
[TABLE]
where is the sheaf on defined by and otherwise. By (2) this gives a long exact sequence of homology groups
[TABLE]
We can identify the complex with the complex , and we have , so that in particular . The homology groups are well known (Folkman66; Bjorner82; Orlik-Terao92) and it follows that
[TABLE]
From this, Proposition 4 and the long exact sequence above, we immediately get vanishes in the degrees . In low degree and top degree we get short exact sequences from which the homology in degree zero and are easily shown to be as claimed. ∎∎
4.4 Cellular homology and broken circuits
To a geometric lattice one can associate a simplicial complex , the broken circuit complex (see MR0453579; MR468931; MR2383131) that encodes some of the combinatorial geometry of the lattice. In this section we outline some connections between and the sheaf homology of . Our description of follows MR2383131*Lectures 3-4.
Let be a geometric lattice and fix a total ordering of the atoms . Label the covering relation , using the atoms, by defining
[TABLE]
where is the maximum atom, with respect to the total order , with the property that . The function (8) is an example of a -labelling. The broken circuit complex has vertices and -simplicies the whenever there is a saturated chain
[TABLE]
with and . Such a chain is said to be -increasing. The resulting depends on the choice of total order , but it turns out that its homotopy type does not. Figure 3 illustrates these ideas for the partition lattice .
The number of -increasing chains (9) is equal to and is a so-called “no-broken-circuit base” for the interval . It is not hard to see that is a pure -dimensional simplicial complex, and that any maximal dimensional simplex contains the vertex that is maximal in the total ordering of . In particular, is a cone whose base is called the reduced broken circuit complex .
Since is a cone, it is contractible, and thus has trivial reduced homology. On the other hand the reduced broken circuit complex has reduced homology
[TABLE]
where
[TABLE]
is the beta-invariant; see MR0572989; MR1165544. Comparing this to Theorem 4.1, it is then very natural to ask what, if any, is the relationship between the sheaf homology of equipped with the natural sheaf and the reduced broken circuit complex? We are grateful to the referee for pointing this out.
It is possible to make a very explicit connection between the sheaf homology of equipped with the constant sheaf and the (un-reduced) broken circuit complex. In order to do this it is most convenient to pass via the “cellular homology” of with coefficients in a sheaf (see EverittTurner15 – suitably adapted to be homological rather than cohomological) and we now briefly explain these ideas.
Let and be a sheaf on . Filter by rank, defining ; the “” is because we are using the -rank function for . Then, is a subcomplex of with quotient complex that we denote by . The cellular chain complex has chains
[TABLE]
and differential provided by the boundary map that arises in the long exact sequence of the triple of subposets . By EverittTurner15*Theorem 2 and §4.4 the cellular chain complex computes sheaf homology:
[TABLE]
After a little analysis, the arguments of EverittTurner15*§2 and §4.4 can be massaged to show that
[TABLE]
where
[TABLE]
with the middle term the ordinary reduced homology of the nerve of . This is in turn free of rank the Möbius function of by Folkman66. It is also possible to give an explicit presentation for the abelian group . Let be a set of linearly independent (in the sense of §1.3) atoms for such that , and consider the saturated chain
[TABLE]
Any other saturated chain has the form
[TABLE]
for a unique . The group is freely generated by elements of the form
[TABLE]
where is -increasing Bjorner82.
Proposition 5
If is a -increasing chain as above with , then the map
[TABLE]
induces an isomorphism from to the simplicial chain complex of .
The homology itself is uninteresting but using cellular homology in this way, makes a fairly direct link between the different chain complexes computing it.
Despite the encouraging start in Proposition 5, this situation we are asking about is different: on one side the constant sheaf should be replaced by the natural sheaf and on the other side the unreduced broken circuit complex should be replaced by the reduced one. These are modifications of quite a different nature: the reduced broken circuit complex may be defined for any lattice (but no sheaf is present) and the natural sheaf is a construction only defined for hyperplane arrangements. It may be possible, to choose bases for the hyperplanes, in such a way that the combinatorics can be pushed to give an isomorphism of chain complexes similar to the one in Proposition 5 in this situation too, but this is not obvious and may well be rather artificial. It would take us too far astray from the purpose of this paper (namely, to present a nice basis-free property of sheaf homology for graded atomic lattices) to attempt this here.
References
