Cohomology on the centric orbit category of a fusion system
Abstract.
We study here the higher derived limits of mod cohomology on the centric orbit category of a saturated fusion system on a finite -group. It is an open problem whether all such higher limits vanish. This is known in many cases, including for fusion systems realized by a finite group and for many classes of fusion systems which are not so realized. We prove that the higher limits of vanish provided , by showing that the same is true for the contravariant part of a simple Mackey composition factor of under the same conditions.
2020 Mathematics Subject Classification:
Primary 55R35, 20E25, Secondary 20J06, 20D20, 55R401. Introduction
The purpose of this note is to show that , considered as a contravariant functor on the centric orbit category of a saturated fusion system on a -group, has vanishing higher derived limits provided .
Theorem 1.1.
Fix a prime and a nonnegative integer . For each saturated fusion system on a finite -group,
for all .
Here denotes the full subcategory of with objects the -centric subgroups, and denotes the corresponding orbit category. For example, the special case of Theorem 1.1 states that the functor is acyclic when is odd. This was a case that motivated our work for reasons we outline below. But first we give context for this result, referring to [BLO03, Section 2] and [AKO11, Section III.5.6] for further details.
One way to study the classifying space of a finite group at a prime (or of a compact Lie group, or of a saturated fusion system over a -group) is to recognize the space as glued from classifying spaces of collections of proper subgroups. Following Dwyer’s uniform approach to such homotopy decompositions in the 1990s [Dwy97], this comes in the form of a map
inducing an isomorphism in mod cohomology, where is a small category and is some functor such that for each , the composite identifies with the classifying space of a subgroup of up to homotopy. The decomposition most relevant here is the subgroup decomposition for the centric collection [Dwy97]. In this case, is the full subcategory of the orbit category of on the -centric subgroups, and is an appropriate lifting to of the classifying space functor to the homotopy category. For example, one can use , the Borel construction applied to the orbit considered as a -space [BS08, Section 5.2].
On the other hand, if is a saturated fusion system on a -group , there may be no finite group with Sylow -subgroup realizing the fusion in (i.e., may be exotic). Consequently there is no longer an obvious lifting of the classifying space functor. As was noticed by Broto, Levi, and Oliver [BLO03, §2], the Dwyer-Kan obstructions to such a lifting [DK92] are the same as the obstructions to the existence and uniqueness of a centric linking system associated with . By a theorem of Chermak, these obstructions vanish [Che13], and the -completion is then regarded as a classifying space “” for the fusion system. The subgroup decomposition in this context takes the form of a mod cohomology isomorphism , where is the left homotopy Kan extension along the quotient functor of the constant functor [AKO11, Proposition III.5.29].
The most immediate application of the subgroup decomposition for a saturated fusion system is to the computation of cohomology of the linking system. The mod cohomology of the linking system is the abutment of the Bousfield-Kan spectral sequence for the homotopy colimit with page given by . Note that by a general property of -local functors on orbit categories, this page is bounded to the right [BLO03, Corollary 3.4]. It is an open problem whether the functor is acyclic, i.e., whether for all . For example, see [AO16, Problem 7.12] and [DP15, Conjecture]. Dwyer called a homology decomposition with this property “sharp”. Sharpness would immediately yield the most natural application of the subgroup decomposition, which is that the cohomology of the linking system satisfies a Cartan-Eilenberg stable elements formula:
The stable elements formula was already shown by Broto, Levi, and Oliver [BLO03, Theorem 5.8] (along with other important consequences for combinatorial descriptions mapping spaces), but the proof relies on difficult results from homotopy theory. It would be very nice to see the stable elements formula directly via sharpness of the subgroup decomposition.
Sharpness over the centric -orbit category of a finite group was shown by Dwyer [Dwy98, §10], and over the centric orbit category of by Díaz and Park [DP15, Theorem B]. Sharpness has since been established for certain families of exotic fusion systems, notably: those on -groups with an abelian subgroup of index [DP15], the smallest Benson-Solomon fusion system [HLL23], all fusion systems of characteristic -type/local characteristic (in the sense of the CFSG) [HLL23], and for the 27 exotic fusion systems on the Sylow -subgroup of [GM22]. The sharpness problem has been studied from a very general point of view also by Yalçın [Yal22], who showed that sharpness for the subgroup and the normalizer decompositions are equivalent.
We follow Díaz and Park [DP15] by regarding cohomology as a Mackey functor for the fusion system, and we study the simple Mackey functors occurring as composition factors of . Theorem 1.1 is ultimately deduced from the following stronger result. We write for short.
Theorem 1.2.
Fix a saturated fusion system on a -group , a subgroup , and a simple -module . If the simple Mackey functor is a composition factor of and , then the restriction of the contravariant part of has vanishing higher derived limits.
Theorem 1.2 is amenable to the standard technique of “pruning”, where one filters by subquotient functors (not themselves contravariant parts of Mackey functors) that take the value except on a single -conjugacy class of subgroups of . Thus, our proof of Theorem 1.1 goes by filtering first as a Mackey functor completely, and then second as a coefficient system.
One reason for our looking at this problem grew out of a loose analogy with the paper [GL16], where we studied higher limits of the center functor -mod, in the context of Oliver’s proof [Oli13] of Chermak’s Theorem [Che13] on centric linking systems. That proof proceeds by a reduction to the case where is realizable by a finite -constrained group with normal centric -subgroup . The observation of [GL16] was the relevance of finding a -local subgroup of that controls fixed points on , i.e. that satisfies , a problem that had been studied by the first author under the guise of “control of weak closure of elements”. This motivated us to look at whether techniques for “controlling transfer” in finite groups could be useful in studying the higher limits of the functor and its subfunctor . The issue is that it appears difficult to get reductions similar to those for the center functor in order for these techniques to be applicable. Also, general techniques for controlling transfer are known only when , so in the end what Theorem 1.1 gives in the case is stronger than what those methods seemingly would have yielded even if they had been applicable.
We would like to thank Antonio Díaz for corrections and helpful suggestions on a previous version of this article.
2. Background results
2.1. Nilpotent action on group cohomology
Let be a commutative ring with identity. If is a finite group, is a subgroup of , and is a -module, then we use the usual notation for fixed points and the relative trace map. If is a rational prime which is zero in , then the relative trace is zero in cases where there is an element of outside but normalizing and acting with small nilpotence degree on . We state this when , the only case we need.
Lemma 2.1.
Let be a finite group, a prime, and an -module. Suppose is an element of of -power order such that . Then for every subgroup of with .
Proof.
Decompose . For each , we have
∎
In this paper, if and are two subsets of a group , we write for the subgroup of generated by the set of commutators with and . Our iterated commutators are right-associated: set , and inductively for . If has a left action on some module , the notation should be interpreted in the semidirect product of by , in which case is a subspace of , and for all and .
The techniques we have generally take advantage of situations in a finite -group in which some subgroup normalizes another subgroup and acts with small nilpotence degree on it, usually action which is quadratic (or trivial): . Then the following lemma of Miyamoto [Miy81, Lemma 2] provides a bound on the nilpotence degree of the action of on that is linear in when is finite abelian.
Lemma 2.2.
Let be a finite -group, a finite abelian group with trivial -action, and a finite group acting on and . Assume and are nonnegative integers such that acts as zero on each -composition factor of , and such that acts as zero on each -composition factor of . Then for all , acts as zero on each -composition factor of .
2.2. Mackey functors for fusion systems
The notation we use for fusion systems follows [AKO11]. We apply morphisms from right to left. Let be a saturated fusion system on a finite -group . A subgroup of is fully -normalized (respectively, fully -centralized) if (respectively, ) for each conjugate of in , i.e., for each subgroup of the form with . A subgroup of is -centric if , i.e. , for each -conjugate of . The symbol denotes the set of -centric subgroups, and also the full subcategory with the same objects. Note that a subgroup of is -centric if and only if it is fully centralized and contains its centralizer in [AKO11, Definition I.3.1]. By one of the axioms for saturation, a fully normalized subgroup is also fully centralized and fully automized: is a Sylow -subgroup of [AKO11, Proposition I.2.5].
For each pair of subgroups , acts on by left composition. The orbit category of is the category with the same objects as and with morphism sets
the orbits under this action. If is a collection of subgroups of which is closed under -conjugacy and also closed under passing to overgroups in , then we abuse notation by using also for the full subcategory of with object set , and we write for the corresponding orbit category. Other than the full orbit category itself, we will only need to work with the centric orbit category, the case .
Since the morphisms in a fusion system model conjugation of -subgroups in a finite group, it is natural that there is a notion of Mackey functor for fusion systems. We first want to recall from [DP15, Section 2] the definition of a Mackey functor in this setting in the form that is most useful later. Let be a commutative ring with identity. Let be a pair of functors from to with contravariant and covariant. Set , , and for each and each isomorphism in . Then is a Mackey functor for if the following conditions hold [DP15, Definition 2.1, Proposition 2.2].
-
(1)
for each ,
-
(2)
(Isomorphism) for each isomorphism in , and
-
(3)
(Mackey formula) for each ,
A morphism of Mackey functors is a family of -module homomorphisms such that is both a natural transformation from and a natural transformation simultaneously. A subfunctor of is a subfunctor of which is simultaneously a subfunctor of , and quotient functors are defined objectwise.
2.3. Simple Mackey functors
The simple objects in are parametrized by pairs , where is a subgroup of taken up to -conjugacy, and where is a simple (irreducible) -module taken up to isomorphism [DP15, Section 3]. When convenient we view as a -module via inflation. The corresponding simple Mackey functor has the property that and for all subgroups such that is not -conjugate to a subgroup of .
Let and let be a simple -module. We give the description of the functor on objects and isomorphisms in from p.153 of [DP15], since this will be important for the proof of Theorem 1.1, but interestingly the effect of on nonisomorphisms is not so important for our argument. For that we refer the interested reader to the description in [DP15]. Our treatment is a little different from (but equivalent to) that in [DP15], since we need to pay somewhat closer attention to precisely how decomposes as a direct sum of -modules.
The set is an - biset with action on either side given by composition. The orbits are in correspondence with the set of subgroups of that are -conjugate to . Likewise the double orbits are in correspondence with the -orbits of such subgroups. Let
be a set of representatives for the double orbits.
For each , we temporarily set and denote (formally) by the -module, isomorphic to as a -module via , with action
for each and . Since acts trivially on , acts trivially on . Set
(2.3) |
the image of the relative trace, where here acts on the -module through the composite
with acting trivially. Note is a -submodule of . It has the structure of a -module on which acts trivially.
Write for the -conjugacy class of , and for the stabilizer of this class in . Since is a normal subgroup of that acts transitively on ,
By construction, the subgroup acts trivially on , and we may regard as a module for via the composite
Set now
(2.4) |
where runs over a set of representatives for the left cosets of in . Then is a -module, that is, still acts trivially. The value of on the subgroup is then
(2.5) |
an -invariant direct sum decomposition.
Now let be another subgroup of and an isomorphism in . The bijection determines the -module isomorphism intertwining the actions of and with respect to conjugation by . It induces an isomorphism of -modules
(2.6) |
intertwining the actions of and . The component of at is the corresponding map of induced modules
and is the sum of these maps.
Note that if is a simple -module, then takes values in -mod. Further, since is simple, is a simple functor [DP15].
2.4. Higher limits of functors on orbit categories
Let be a commutative -algebra and let be a contravariant functor from the orbit category of a group or a fusion system to the category of -modules. A common technique for computing the higher limits of (and especially for showing that such higher limits vanish) is to use a filtration of each of whose successive quotient functors is atomic, namely a functor which vanishes except on a single conjugacy class of subgroups. This method does not always work as, for example, in the case of the center functor [Oli18]. But the idea is often effective for making reductions even when it doesn’t work directly. And ultimately it is all that is needed for the proof of the main theorem here.
Let be a finite group and let be a -module. Define a functor
via and when . The action of on is the given one. The higher limits of are denoted and arise as the higher limits of atomic functors, as was first shown by Jackowski, McClure, and Oliver [AKO11, Proposition 5.20].
Proposition 2.7.
Let be any functor on the orbit category of a fusion system which vanishes except on the -conjugacy class of a subgroup . Then there is an isomorphism .
Let be a set of representatives for the -conjugacy classes of subgroups of such that if , then is not conjugate to a subgroup of . Then one can make a filtration , in which is the functor equal to on the union of the conjugacy classes with , and otherwise. Then if is conjugate to , and it is zero otherwise, i.e. the quotient is atomic.
In general, we use the notation for the atomic subquotient functor of corresponding to the -conjugacy class of , namely the functor with values if is -conjugate to , and otherwise.
The next lemma is proved using long exact sequences on higher limits corresponding to short exact sequences of functors arising out of a filtration of the above type.
Lemma 2.8 ([AKO11, Corollary 5.21(a)]).
Let be a contravariant functor on the centric orbit category of a fusion system . Assume that is acyclic for all , i.e., for all . Then is acyclic.
The functors vanish in many cases. See for example Section III.5 of [AKO11] for many results along these lines. In the next lemma we state two such vanishing results.
Recall that a radical -chain of length in the finite group is a sequence such that for each , where here denotes the intersection of the normalizers in of the .
Lemma 2.9.
Let be a finite group, a -module, and .
-
(1)
If , then .
-
(2)
If for each radical -chain of length in , then .
Proof.
We want to show (Theorem 1.2) that the restriction of the contravariant part of each Mackey composition factor of is acyclic when . For doing this, Díaz and Park show we can restrict attention to composition factors with not -centric.
Lemma 2.10.
Let be a field of characteristic and a saturated fusion system on the finite -group . For each -centric subgroup and each simple -module , the restriction of the contravariant part of is acyclic.
3. Proof of Theorem 1.1
Throughout this section we fix a prime , and a saturated fusion system on the -group . We set for short. For fixed , we consider as a Mackey functor on where the contravariant structure is induced by restrictions and conjugations, and where the covariant structure is induced by transfers and conjugations (as usual).
We first fix some additional notation that we keep for the remainder of the section.
Let be the collection of all normal subgroups of such that
(3.1) |
By [Gor80, 5.3.12], each subgroup maximal subject to being normal and abelian coincides with its centralizer in . Since , we have . Thus, is nonempty. Further, since each member of is normal in , it is fully normalized, hence fully centralized by one of the saturation axioms for . This implies .
Definition 3.2.
Let be a subgroup of . Define to be the set of pairs consisting of a centric subgroup and a morphism having the property that there are and an isomorphism in such that .
The proof of Theorem 1.1 is broken into two propositions. In the first one, we show that the -submodule of (see equation (2.4)) is 0 whenever is a composition factor of , , and . In the second one, we use this to show that the atomic subquotient is acyclic for an arbitrary -centric subgroup when is not -centric.
Proposition 3.3.
Fix a prime , a saturated fusion system on a finite -group , a nonnegative integer , a subgroup , and a simple -module . If and is a composition factor of , then for all .
Proof.
Let . By Definition 3.2 there is an -isomorphism and such that for , we have . The map induces an intertwining . Because of this we may as well change to lighter notation by replacing by , by , and by . Thus, and we want to show .
Set for short. Since is normal in , is normal in and is normal in . Also, as , we have . Hence . Since is a composition factor of , is a -composition factor of , and is an -composition factor of . We have ; in particular acts quadratically on every -composition factor of . The hypotheses of Lemma 2.2 thus hold with and , and with , , and in the roles of , , and . As is a composition factor of , by that lemma we have for all . Since composition factors are always -vector spaces and , Lemma 2.1 implies . Hence
and this completes the proof. ∎
Proposition 3.4.
Fix a prime , a saturated fusion system on a finite -group , and a nonnegative integer . Let be a composition factor of such that is not -centric. If , then for all , the atomic subquotient functor is acyclic.
Proof.
Fix . The functor does not depend on , but only on the -conjugacy class of . By Proposition 2.7, we have
for any -conjugate of . So we may assume to be fully normalized in . In particular, is a Sylow -subgroup of . By Lemma 2.9(1), the proposition holds if , so we are reduced to .
Adopt the notation of Section 2.3. By (2.5) and additivity of the functors , we have
(3.5) |
Fix arbitrary and . Set and for short, and let .
Since is not -centric, and are not -centric, and . Thus , and so . As is normal in , is normal in . Let be a normal subgroup of minimal subject to . Since normalizes and is normal in , we have , and hence
for each . That is,
(3.6) |
for each .
Fix a radical -chain of with , and let be its normalizer. Conjugating in in order to take , we will show that the hypotheses of Lemma 2.9(2) hold for the conjugate chain, and then conjugating back, it holds for the one just fixed. In this way we are reduced to .
Let be arbitrary. Recall that was chosen so that is a minimal normal subgroup of (contained in . As a minimal normal subgroup of a finite -group, is therefore of order and contained in the center of , the last equality because . Thus, . Since , we have by (3.6), and so as is abelian. In particular, for every -composition factor of . As is an -composition factor of , we have
for all |
by Lemma 2.2 applied with , , , , and in the roles of , , , and . So for all as is a -submodule of . Since this holds for all , we have by the direct sum decomposition (2.4) that
Lemma 2.1 now applies with in the role of , with in the role of , and with a generator of . As , we have by that lemma. Therefore, Lemma 2.9(2) and (3.5) combine to give . ∎
Proof of Theorem 1.2.
Let be a composition factor of as a Mackey functor on , and suppose that . If is centric, then is acyclic by Lemma 2.10. If is not -centric, then Proposition 3.4 shows that the atomic functor is acyclic for each , so again is acyclic by Lemma 2.8. ∎
Proof of Theorem 1.1.
As made explicit in the proof of [DP15, Proposition 4.3], given a filtration of whose successive quotients are simple Mackey functors for , the restrictions to of the contravariant parts of the members of the filtration yield a filtration for . So the theorem follows from Theorem 1.2. ∎
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