$A_1$-type subgroups containing regular unipotent elements
Timothy C. Burness, Donna M. Testerman

TL;DR
This paper proves that most subgroups of a simple exceptional algebraic group containing a regular unipotent element are contained within an $A_1$-type subgroup, extending previous results and with specific notable exceptions.
Contribution
It generalizes earlier work by showing that such subgroups are contained in $A_1$-type subgroups, except for two specific cases involving $E_6$ and $E_7$ with particular primes.
Findings
Most subgroups with regular unipotent elements are contained in $A_1$-type subgroups
Two specific exceptions identified for $(E_6,13)$ and $(E_7,19)$
Applications to subgroup structure of finite groups of Lie type
Abstract
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic and let be a subgroup of containing a regular unipotent element of . By a theorem of Testerman, is contained in a connected subgroup of of type . In this paper we prove that with two exceptions, itself is contained in such a subgroup (the exceptions arise when or ). This extends earlier work of Seitz and Testerman, who established the containment under some additional conditions on and the embedding of in . We discuss applications of our main result to the study of the subgroup structure of finite groups of Lie type.
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.
Taxonomy
TopicsFinite Group Theory Research · graph theory and CDMA systems · Coding theory and cryptography
-type subgroups containing regular
unipotent elements
Timothy C. Burness
T.C. Burness, School of Mathematics, University of Bristol, Bristol BS8 1TW, UK
and
Donna M. Testerman
D.M. Testerman, Institute of Mathematics, Station 8, École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
Abstract.
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic and let be a subgroup of containing a regular unipotent element of . By a theorem of Testerman, is contained in a connected subgroup of of type . In this paper we prove that with two exceptions, itself is contained in such a subgroup (the exceptions arise when or ). This extends earlier work of Seitz and Testerman, who established the containment under some additional conditions on and the embedding of in . We discuss applications of our main result to the study of the subgroup structure of finite groups of Lie type.
2010 Mathematics Subject Classification:
Primary 20G41; Secondary 20E32, 20E07
1. Introduction
Let be a simple algebraic group of adjoint type over an algebraically closed field of characteristic . Let be a subgroup of , where is a -power, and let be an element of order . By the main theorem of [26], is contained in a closed connected subgroup of of type , unless , and belongs to the conjugacy class of labelled as in [14]. With a view towards applications to the study of the subgroup structure of finite groups of Lie type, it is desirable to seek natural extensions of this result. In particular, under what conditions can one embed the full subgroup in an subgroup of ?
As a special case of the main theorem of [29], this question has a positive answer when is classical and is not contained in a proper parabolic subgroup of (for , this is a well-known theorem of Steinberg [32]). One can see that the condition on the embedding of is necessary by considering indecomposable representations of which do not arise as restrictions of indecomposable representations of an algebraic . In [29], Seitz and Testerman also provide a positive answer if is a simple exceptional algebraic group (of type , , , or ) and is large enough, still under the same assumption that is not contained in a proper parabolic subgroup of . More precisely, the approach in [29] requires where
[TABLE]
More general results on the embedding of finite quasisimple subgroups in exceptional algebraic groups are established by Liebeck and Seitz in [18]. For instance, if and is sufficiently large, then [18, Theorem 1] implies that is contained in a proper closed positive dimensional subgroup of . Here “sufficiently large” means that with
[TABLE]
It is natural to seek an extension of [29, Theorem 2] by removing the conditions on and the embedding of in when is of exceptional type and . In [30], Seitz and Testerman study the case where is semiregular in (that is, is a unipotent group). Notice that if is not semiregular then for some non-trivial semisimple element and one can hope to answer the question in the proper reductive subgroup ; so the semiregular case, where such a reduction is not possible, is particularly interesting. In this situation, the main result of [30] states that is contained in a connected subgroup of type if either , or if and .
In this paper, we extend the results in [30] by studying the remaining case where and . In order to do this, we will assume is regular in , which means that is an abelian unipotent group of dimension , where is the rank of (equivalently, is contained in a unique Borel subgroup of ). It is well known that regular unipotent elements exist in all characteristics and they form a single conjugacy class. Since the order of is the smallest power of greater than the height of the highest root of (see [35, Order Formula 0.4]), our hypothesis implies that , where is the Coxeter number of . (Recall that , where is the height of the highest root of .)
Our main result is the following (in this paper, an -type subgroup is a closed connected subgroup isomorphic to or ).
Theorem 1**.**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of . Then exactly one of the following holds:
- (i)
* is contained in an -type subgroup of ;*
- (ii)
, and is contained in a -parabolic subgroup of ;
- (iii)
, and is contained in an -parabolic subgroup of .
In all three cases, is uniquely determined up to -conjugacy.
Remark 1**.**
Let us make some comments on the statement of Theorem 1.
- (a)
To see the uniqueness of in part (i), it suffices to show that every subgroup of containing is conjugate to . Write and , where and are -type subgroups of . By Proposition 2.11(ii), and are -conjugate, say , so . Finally, by applying [17, Theorem 5.1] and Lang’s theorem, we deduce that and are -conjugate.
- (b)
The interesting examples arising in (ii) and (iii) were found by Craven [9] in his recent study of the maximal subgroups with socle in finite exceptional groups of Lie type. The action of such a subgroup on the adjoint module is described in Theorem 8.1 (see Section 8) and its construction is explained in [9, Section 9]. Let us say a few words on the construction in (ii), where and . Let be a -parabolic subgroup of and identify the unipotent radical with a -dimensional spin module for . Take a subgroup containing a regular unipotent element of and consider the semidirect product (note that is uniquely determined up to -conjugacy). Now one checks that has an -dimensional composition factor with , which is a direct summand of . It follows that there is a complement to in that is not -conjugate to . Moreover, one can show that contains a regular unipotent element of and there is a unique -class of such subgroups (hence is uniquely determined up to -conjugacy). We will show that the subgroup constructed in this way is not contained in an -type subgroup of (this follows from Theorem 2 below). A similar construction can be given in (iii) and again one can show that such a subgroup is both unique up to conjugacy and is not contained in an -type subgroup.
- (c)
The conclusion of Theorem 1 for can be deduced from the proof of [30, Lemma 3.1]. It also follows from Kleidman’s classification of the maximal subgroups of in [13]. However, for completeness we will provide an alternative proof, following the same approach we use for the other exceptional groups.
- (d)
Finally, let us comment on the adjoint hypothesis in the statement of the theorem. Let be a simple exceptional algebraic group and let be the corresponding adjoint group. Suppose or is a subgroup of containing a regular unipotent element of . The regularity of implies that and thus is a subgroup of containing a regular unipotent element, so it is determined by Theorem 1.
The next result shows that the subgroups in part (i) of Theorem 1 are -irreducible in the sense of Serre (that is, is not contained in a proper parabolic subgroup of ). The proof is given at the end of Section 2. By [36, Theorem 1.2], any connected reductive subgroup of a reductive algebraic group containing a regular unipotent element is -irreducible, so we can view Theorem 2 as a partial analogue for subgroups isomorphic to in simple exceptional groups.
Theorem 2**.**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic and let be a regular unipotent element such that
[TABLE]
where is an -type subgroup of . Then is -irreducible.
Remark 2**.**
As in Theorem 1, let be a subgroup of containing a regular unipotent element. By combining Theorems 1 and 2, we deduce that is contained in an -type subgroup of if and only if is not contained in a proper parabolic subgroup of . In particular, the examples arising in parts (ii) and (iii) of Theorem 1 are genuine exceptions to the containment in (i).
The next result follows by combining Theorem 1 with the main results of [29, 30].
Corollary 1**.**
Let be a simple algebraic group of adjoint type over an algebraically closed field of characteristic and let be a subgroup of containing a regular unipotent element of , where is a -power. In addition, if is classical assume that is -irreducible. Then either
- (a)
* is contained in an -type subgroup of , or*
- (b)
* and is one of the cases in parts (ii) and (iii) in Theorem 1.*
Next we present some further applications of Theorem 1. Let be a simple algebraic group as in Theorem 1 and recall that a finite subgroup of is Lie primitive if
- (a)
does not contain a subgroup of the form , where is a Steinberg endomorphism of with fixed point subgroup ; and
- (b)
is not contained in a proper closed subgroup of of positive dimension.
In [11, Section 3], Guralnick and Malle determine the maximal Lie primitive subgroups of containing a regular unipotent element (the maximal closed positive dimensional subgroups of containing a regular unipotent element were determined in earlier work of Saxl and Seitz [27]). More precisely, they give a list of possibilities for , but they do not claim that all cases actually occur. In particular, their proof relies on [29] and thus arises as a possibility when and , where is the integer in (1). Therefore, by combining [11, Theorems 3.3, 3.4] with Theorem 1, we obtain the following refinement.
Corollary 2**.**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic . Suppose is a maximal Lie primitive subgroup of containing a regular unipotent element. Let denote the socle of .
- (i)
If , then one of the following holds:
- (a)
* and ;*
- (b)
* and , or ;*
- (c)
* and .*
- (ii)
If , then one of the following holds:
- (a)
* and , or ;*
- (b)
* and , or , or .*
- (iii)
If , then one of the following holds:
- (a)
* and , or ;*
- (b)
* and either or .*
- (iv)
If , then and or .
- (v)
If , then one of the following holds:
- (a)
* and ;*
- (b)
* and or ;*
- (c)
* and or , or , or .*
Remark 3**.**
By Corollary 2, there are no Lie primitive subgroups containing a regular unipotent element if . This lower bound is best possible: the case with is a genuine example (this can be deduced from recent work of Litterick [22]). However, we are not claiming that all of the possibilities listed in Corollary 2 are Lie primitive and contain regular unipotent elements (indeed, we expect that this list can be reduced further).
We can also use Theorem 1 to shed new light on the subgroup structure of finite exceptional groups of Lie type. Let be a simple exceptional algebraic group of adjoint type over with prime and let be a Steinberg endomorphism of with fixed point subgroup , an almost simple group over . The maximal subgroups of the Ree groups and (and their automorphism groups) have been determined up to conjugacy by Kleidman [13] and Malle [23], respectively, and similarly is handled in [8] for even and in [13] for odd. Therefore, we may assume is one of , , , and . In these cases, through the work of many authors, the problem of determining the maximal subgroups of has essentially been reduced to the case where is an almost simple group of Lie type with socle over a field of characteristic (see [24, Section 29.1] and the references therein). Here one of the main problems is to determine if such a subgroup is of the form , where is maximal among positive dimensional -stable closed subgroups of . Significant restrictions on the rank of and the size of are established in [16, 18], but the problem of obtaining a complete classification is still open.
The case is of particular interest. If , where is the integer in (2), then the aforementioned work of Liebeck and Seitz [18] shows that and for some maximal connected subgroup of of type . Further results in this direction have recently been obtained by Craven [9] when is one of , , or . Using the maximality of , he proves that in almost every case, but his approach is unable to eliminate certain values of . In particular, the case where contains a regular unipotent element of is problematic (the existence of such subgroups, in a much more general setting, was established by Serre [31], which explains why they are called Serre embeddings in [9]). Using Theorem 1, one can show that all maximal Serre embeddings are of the form (we can also handle , which is excluded in [9]). In particular, it follows that part (1) in [9, Theorem 1.2] is a subcase of part (2), and similarly part (2) in [9, Theorem 1.4] is a subcase of part (3).
To conclude the introduction, let us briefly describe the main steps in the proof of Theorem 1 (we refer the reader to Section 2.5 for more details). Suppose is a regular unipotent element of and let be an -type subgroup containing with maximal torus . Set and . Without loss of generality, replacing by a suitable -conjugate, we show that we may assume contains the toral element , which corresponds to a diagonalizable element with eigenvalues and (see Lemma 2.19). We can use the known action of on to determine the eigenvectors and eigenspaces of on and this severely restricts the possibilities for . It is possible to obtain further restrictions on the indecomposable summands of by considering the trace on of semisimple elements in of small order (typically, we only need to work with elements of order and ).
In this way, in almost all cases, we are able to reduce to the situation where is compatible with the action of a subgroup of . In this situation, is given in Table 2 (our notation for indecomposable summands in Table 2 is explained in Section 2.1) and we observe that the socle of has a -dimensional simple summand
[TABLE]
where is an eigenvector for with eigenvalue . Let be the -eigenspace of on . Without loss of generality, we may assume that the action of on (in terms of this basis) is given by the matrix
[TABLE]
and thus
[TABLE]
Our main goal is to show that is an -subalgebra of .
To do this, we may assume that is obtained by exponentiating the regular nilpotent element with respect to a fixed Chevalley basis
[TABLE]
for (see Section 2.5 for more details). This allows us to explicitly identify a maximal torus of an -type subgroup of containing , which means that we can compute eigenvectors and eigenspaces for in terms of the Chevalley basis. With the aid of Magma [3] to simplify the computations, we can describe the action of on in terms of a matrix with respect to and then compute bases for the subspaces for . In this way, we obtain expressions for and in terms of , but with undetermined coefficients. We then derive relations between these coefficients by considering the action of on , and further relations can be found by using the fact that is an abelian subalgebra. Apart from a handful of special cases, this allows us to reduce to the case where is an -subalgebra and we complete the argument by showing that the stabilizer of in is an -type subgroup.
This process of elimination and extension comprises the bulk of the proof of Theorem 1 (see Sections 3–7). However, there are a handful of possibilities for which require further attention; these are the cases arising in part (ii) of Theorem 2.23 and they are handled in Section 8. In each of these cases, the action of on is known (up to one of three possibilities if or ) and stabilizes a non-zero subalgebra of . This allows us to reduce to the case where is contained in a proper parabolic subgroup of . Let be the quotient map. Using , we identify with and so we may view as a subgroup of . We may as well assume that is a minimal parabolic (with respect to containing ), so is not contained in a proper parabolic subgroup of . Now is a regular unipotent element which is contained in an -type subgroup of (this follows by combining Theorem 2.23 with the aforementioned earlier work of Seitz and Testerman [29] for classical groups). By inspecting [15], we can determine the action of on , which must be compatible with the action of on given in Theorem 2.23. In this way we deduce that and are the only possibilities, and this completes the proof of Theorem 1.
Notation
Our notation is fairly standard. For a simple algebraic group we write , and for the set of roots, positive roots and simple roots of , with respect to a fixed Borel subgroup, and we follow Bourbaki [4] in labelling the simple roots. We will often denote a root by writing . If is a module for a group then and denote the socle and radical of , respectively, and we write to denote (with summands). It will be convenient to write for a block-diagonal matrix with a block occurring with multiplicity . In addition, we will write for a standard (upper triangular) unipotent Jordan block of size .
2. Preliminaries
In this section we record some preliminary results that will be needed in the proof of Theorem 1. We start by recalling some well known results from the modular representation theory of the simple groups . Our main reference is Alperin [1].
2.1. Representation theory
Let be an algebraically closed field of characteristic , let and let be a Sylow -subgroup of .
The subgroup of has exactly indecomposable -modules, say for , where and is the unique projective indecomposable -module. The element has Jordan form on . In particular, if is a projective -module, then for some , and has Jordan form on .
There are precisely simple -modules, labelled in [1], where . In particular, every simple -module is odd-dimensional. Here is the trivial module and is the Steinberg module. It is easy to see that has Jordan form on . By a theorem of Steinberg, each is the restriction of a simple module for the corresponding algebraic group of type (see [33, Section 13]), so we can refer to the highest weight of with respect to a maximal torus of the algebraic . We identify the weights of this -dimensional torus with the set of integers, and we will often write to highlight the highest weight of .
Similarly, there are precisely projective indecomposable -modules, labelled in [1], where is simple and the remainder are reducible. Here and for . The element has Jordan form on and , and Jordan form on the remaining . The structure of these modules is described by Alperin [1, pp.48–49]. In terms of composition factors, we have
[TABLE]
and
[TABLE]
where is odd. (Here this notation indicates that and .) It will be convenient to define
[TABLE]
and
[TABLE]
for .
The Green correspondence (see [1, Section 11]) implies that if is an indecomposable -module then where is projective (or zero) and is indecomposable (or zero). In particular, the following lemma holds.
Lemma 2.1**.**
Let be an -dimensional indecomposable -module and write , where and . Then has Jordan form on .
The main result on the structure of indecomposable -modules is the following theorem. Here we define a subtuple of an -tuple to be a tuple of the form for some . We denote this by writing
[TABLE]
Theorem 2.2**.**
Let be a reducible indecomposable non-projective -module. Then there exists an integer and a subtuple
[TABLE]
such that
[TABLE]
where if is even, otherwise .
Proof.
This follows from the discussion in [12, Section 3]. Also see [9, Section 7.3]. ∎
Corollary 2.3**.**
Let be an indecomposable -module with precisely two composition factors. If then for some , hence .
Corollary 2.4**.**
Let be a reducible indecomposable -module. Then . Moreover, if has at least four composition factors, then .
2.2. Traces
As in Section 2.1, let be an algebraically closed field of characteristic and set . Let and be representatives of the unique conjugacy classes of elements of order and in , respectively (note that is semisimple since ). Let be a -module and let denote the trace of on .
Lemma 2.5**.**
If then
[TABLE]
Proof.
This is a straightforward calculation, using the fact that we can identify with the -th symmetric power , where is the natural module for . ∎
If is a -module with composition factors , then
[TABLE]
since the action of is diagonalizable. Therefore, the next two results are immediate corollaries of Lemma 2.5 (here we use the notation and defined in (3) and (4)).
Lemma 2.6**.**
We have
[TABLE]
Lemma 2.7**.**
We have
[TABLE]
and
[TABLE]
Let be a simple algebraic group over of adjoint type, let be a -module and let be a positive integer. Define
[TABLE]
Recall that the adjoint module for is the Lie algebra , on which acts via the adjoint representation.
Proposition 2.8**.**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic . Let be the adjoint module. Then is recorded in Table 1 for .
Proof.
This follows by inspecting the dimensions of the centralizers of elements of order in (see [10, Tables 4.3.1 and 4.7.1]), using the fact that
[TABLE]
for every semisimple element (see [6, Section 1.14], for example).
For instance, if has order and , then and the self-duality of implies that the action of on is given by the diagonal matrix , up to conjugacy, where is a primitive cube root of unity. Therefore, . ∎
Remark 2.9**.**
Suppose is contained in , where and is adjoint. Write and , where is the simply connected group of type and is the centre of . Now has Schur multiplier , which implies that . Therefore, every element of order lifts to an element in of order . In particular, if has order then , or (see [10, Table 4.7.1]), whence with respect to .
Remark 2.10**.**
In a few cases it is helpful to know the eigenvalue multiplicities on of elements in of order for certain values of ; the relevant cases are the following:
[TABLE]
It is straightforward to obtain this information with the aid of Magma [3], using an algorithm of Litterick (see [21, Section 3.3.1]), which is heavily based on work of Moody and Patera [25]. We thank Dr. Litterick for his assistance with these computations.
2.3. -type subgroups
Let be a simple algebraic group and recall that is a good prime for if in types and , for and , and when is of type (all primes are good in type ).
Proposition 2.11**.**
Let be a simple algebraic group of adjoint type over an algebraically closed field of good characteristic . Let be an element of order .
- (i)
There is an -type subgroup of containing .
- (ii)
If is regular then the subgroup in (i) is unique up to -conjugacy.
Proof.
Part (i) follows from the main theorem of [35]. Part (ii), for exceptional, follows from [15, Theorem 4]. Now assume is classical and let be an -type subgroup of containing . Let be the natural module for . By [36, Theorem 1.2], is not contained in a proper parabolic subgroup of . In particular, if is of type or then acts irreducibly and tensor indecomposably (see [36, Proposition 2.3]) on and the conjugacy statement follows from representation theory.
Finally, let us assume (with ). We claim that , where is the stabilizer of a non-singular -space. The result then follows since is unique in up to -conjugacy, and itself is unique up to -conjugacy. To justify the claim, first observe that has Jordan form on , using [27, Lemma 1.2(ii)] and the fact that has order , so . If acts irreducibly on then the Jordan form of implies that is tensor decomposable, but this is incompatible with [27, Lemma 1.5]. Therefore, acts reducibly on and we complete the argument by applying [20, Lemma 2.2]. ∎
Proposition 2.12**.**
Let be a simple exceptional algebraic group of adjoint type and let be a regular unipotent element such that
[TABLE]
where is an -type subgroup. Then the action of on the adjoint module is given in Table 2.
Proof.
A precise description of as a tilting module is given in [19, Table 10.1] (for we may assume that so the action of on can be deduced from the actions of on and the minimal module for (see [19, Table 10.2])). Following [19], we write for a tilting module having the same composition factors as the direct sum of Weyl modules for with highest weights In terms of this notation, we get
[TABLE]
As explained at the start of [19, Section 10], we can express as a direct sum of indecomposable tilting modules of the form , where the highest weight is at most . For example, suppose and , so as above. The highest weight is , so one summand is , which is a uniserial module of shape (see [28, Lemma 2.3]). The highest weight not already accounted for is , so is a summand and we deduce that and thus
[TABLE]
By [28, Lemma 2.3], is a projective indecomposable -module of dimension , so for some . By comparing socles, it follows that and thus
[TABLE]
as recorded in Table 2. The other cases are entirely similar and we omit the details. ∎
For the remainder of this section, let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic , and let and be the rank and Coxeter number of , respectively. We will assume contains a regular unipotent element of order , which means that
[TABLE]
We need to recall the construction of -type subgroups of containing regular unipotent elements, following the treatment in [31, 34, 35].
First we need some new notation. Let be a simple Lie algebra over of type . Fix a Chevalley basis
[TABLE]
of and write for and . It will be convenient to define for each . Let be the -span of and set . (By abuse of notation, we also write for the elements , , etc., in .) Fix a root . As in the familiar Chevalley construction, we have
[TABLE]
for all , and this allows us to construct the element
[TABLE]
where x is an indeterminate. Passing to , we obtain a -dimensional unipotent subgroup
[TABLE]
(see [5, Proposition 4.4.2]). Note that .
Given the lower bound on in (5), we can make a similar construction for more general elements of . To do this, let be the -span of , where is the localization of at the prime ideal , so that . By [35, Proposition 1.5] we have
[TABLE]
for all and all . Then as in the Chevalley construction, for any non-zero element in or , we can produce
[TABLE]
In particular, by passing to , we define
[TABLE]
We will use this general set-up to construct certain -type subgroups of our group , following [34, 35]. In order to state the main result (Proposition 2.13 below), recall that an ordered triple of elements chosen from (or from ) is an -triple if the elements satisfy the commutation relations between the standard generators of the Lie algebra , namely
[TABLE]
We have the following result (in part (iii), we use the notation from (6)).
Proposition 2.13**.**
Suppose and is an -triple of , with and . Then the following hold:
- (i)
* and are -dimensional subgroups of .*
- (ii)
* is an -type subgroup of .*
- (iii)
* is a maximal torus of , where*
[TABLE]
and the map is a morphism of algebraic groups.
- (iv)
The action of on the basis of is given by
[TABLE]
for all , . Moreover, for all .
- (v)
* normalizes and .*
- (vi)
* contains a regular unipotent element of .*
Proof.
This follows by combining Lemmas 1 and 2 in [34] with Lemma 1.2 in [35]. ∎
The following result will play an important role in the proof of Theorem 1.
Proposition 2.14**.**
Suppose and is an -triple of , with and . Let be the -dimensional subalgebra of generated by and let be the stabilizer of in . Then is an -type subgroup of .
Proof.
Let be the -type subgroup of constructed in Proposition 2.13(ii). Note that contains a regular unipotent element and it clearly stabilizes by construction, so . Let be a maximal closed positive dimensional subgroup of with . By the main theorem of [36], is not contained in a proper parabolic subgroup of , so Borel-Tits [2, Corollary 3.9] (also see Weisfeiler [37]) implies that is reductive. By [27, Theorem A], either is an -type subgroup (and thus ), or and . In the latter case, since does not stabilize a -dimensional subspace of , so let be a maximal closed positive dimensional subgroup of with . As above, is reductive and by applying [27, Theorem A] once again, we conclude that . ∎
We would like to be able to use Proposition 2.14 to identify the stabilizers of other -subalgebras of . With this aim in mind, we present Proposition 2.15 below. In order to state this result, we need some additional notation.
Suppose we have an -triple as in Proposition 2.13. Let be the -dimensional torus constructed in part (iii) of the proposition. Let be the highest root and recall that , where is the familiar height function (that is, if then ). Then
[TABLE]
is the set of weights of on both and . For each -weight , write for the corresponding -weight space and similarly for . In both the statement and proof of the following result, we use the notation for .
Proposition 2.15**.**
Suppose and is an -triple of , with and . Suppose and are chosen so that
- (i)
* in ; and*
- (ii)
* is an -triple in for some .*
Then there exists such that and in . Moreover, the stabilizer in of the subalgebra of generated by is an -type subgroup.
Proof.
First observe that since , so we can take as in (6). Note that since . Now is an eigenvector for (since is a -weight vector), so and thus
[TABLE]
The maximum -weight in is , which is at most since , so for all and thus
[TABLE]
In addition, since and , we have
[TABLE]
The commutation relations imply that , which is equal to by (7). Therefore, and thus . We conclude that and in , as required. The final statement concerning the stabilizer of follows immediately from Proposition 2.14. ∎
2.4. Exponentiation
In this section we turn to a different notion of “exponentiation”, following Seitz [28]. As before, let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic and let and denote the rank and Coxeter number of , respectively. Let be the unipotent radical of a fixed Borel subgroup of corresponding to our choice of base , where the root subgroup is defined as in (6). As explained in [28, Section 5], we may view as an algebraic group via the Hausdorff formula. Set .
We start by recalling [28, Proposition 5.3].
Proposition 2.16**.**
Suppose . Then there exists a unique isomorphism of algebraic groups
[TABLE]
whose tangent map is the identity and which is -equivariant; that is, for all , .
Suppose contains a regular unipotent element of order , so and we are in a position to use Proposition 2.16 to study the structure of . Replacing by a suitable conjugate, we may assume that
[TABLE]
where . As in Proposition 2.13, let be an -type subgroup of containing , and let be the given maximal torus of . Without loss of generality, we may assume that is contained in the Borel subgroup defined above. From the description of the action of on in the proof of Proposition 2.12, it follows that acts on the -eigenspace as
[TABLE]
where the are recorded in Table 3 (we label the so that they form a decreasing sequence).
Proposition 2.17**.**
Let be a regular unipotent element of order , where , and let be the torus constructed in Proposition 2.13. Then there exist connected -dimensional unipotent subgroups such that the following hold:
- (i)
. In particular, each can be written as a commuting product of the form for some .
- (ii)
We have
[TABLE]
for all , , .
Proof.
First note that since has order . As above, let
[TABLE]
be the unipotent radical of a Borel subgroup of and note that and . Moreover, we have and thus . Choose such that , where is the map in Proposition 2.16. Extend to a basis of the -eigenspace , where for each , and construct the corresponding connected -dimensional unipotent subgroups
[TABLE]
Recall that is abelian, so is an abelian subalgebra and the proof of [28, Proposition 5.4] implies that each is contained in . Therefore, is a closed connected unipotent subgroup of . Moreover, for each , so and thus (note that is connected since is adjoint). Part (i) now follows since is abelian. Finally, part (ii) follows from the -equivariance of (see Proposition 2.16). ∎
Proposition 2.18**.**
Let be the unipotent radical of a Borel subgroup of , let be a proper non-zero subalgebra of and let be the stabilizer of in . Assume contains a regular unipotent element of of order . Then either
- (i)
* is contained in a proper parabolic subgroup of ; or*
- (ii)
* is contained in an -type subgroup of .*
Proof.
Since , we can consider the isomorphism in (8). Let be the centre of , which is a non-zero abelian subalgebra of stabilized by . We claim that . To see this, let , and note that and commute since in (see the proof of [28, Proposition 5.4]). The -equivariance of implies that
[TABLE]
so and the claim follows. Therefore, is a positive dimensional subgroup of containing a regular unipotent element.
To complete the argument, we proceed as in the proof of Proposition 2.14, using Borel-Tits [2, Corollary 3.9]. Let us assume is not contained in a proper parabolic subgroup of . Then , where is a maximal closed reductive positive dimensional subgroup of . By the main theorem of [27], either is an -type subgroup, or and , so we may assume that we are in the latter situation. Suppose . Since
[TABLE]
where is the minimal module for , it follows that is the only possibility. But must contain non-zero elements in the Lie algebra of a maximal torus of (just by comparing dimensions) and this is a contradiction. Therefore is a proper subgroup of and thus for some maximal closed reductive subgroup of . By a further application of [27] we conclude that is contained in an -type subgroup of . ∎
2.5. Methods
In this section we discuss the proof of Theorem 1, highlighting the main steps and ideas.
Let be a simple exceptional algebraic group of adjoint type defined over an algebraically closed field of characteristic . Let be the rank of and let be the adjoint module. Suppose is a regular unipotent element of , so where is the Coxeter number of . The embedding of in corresponds to an abstract homomorphism with kernel and image .
As before, let be a simple Lie algebra over of type and fix a Chevalley basis
[TABLE]
Since , we can view as a basis for , where are in the appropriate root spaces with respect to the Cartan subalgebra spanned by the . It will be convenient to write for and .
Set and let be an -triple as in Proposition 2.13. Let be the corresponding -type subgroup of constructed in Proposition 2.13, with maximal torus and associated morphism . By replacing by a suitable -conjugate, we may assume that . Let be a morphism of algebraic groups such that
[TABLE]
for all , . We may assume is an isomorphism of algebraic groups.
Consider the elements
[TABLE]
in , where . Without loss of generality, we may assume that so with . Then and thus for some . Set .
Lemma 2.19**.**
There exists a -conjugate of containing and .
Proof.
As noted above, we have for some . By Proposition 2.17 there are scalars such that . Let us consider a general element . In view of (10), we get
[TABLE]
where the are the integers appearing in Table 3.
Since and , it is easy to see that there is at most one such that . If there is no such then we can set for all , so and is the desired conjugate of . Finally, suppose and for some . By defining as above for all , we get with . But this implies that is a non-semisimple element, which contradicts the semisimplicity of . ∎
In view of the lemma, we may assume that contains , which corresponds to a diagonalizable element with eigenvalues and . Since , we can use the known action of on (see the proof of Proposition 2.12) to determine the eigenvectors and eigenspaces of on . For example,
[TABLE]
is the collection of eigenvalues of on , where the are given in Table 3. We set , where is the centre of . Note that contains the Borel subgroup of .
The proof of Theorem 1 has three main steps, which we now describe.
Step 1: Elimination. Our initial aim is to reduce to the situation where the action of on is compatible with the decomposition of as an -module given in Table 2. In almost all cases, we are able to achieve this goal. To do this, we consider the possible decompositions of as a direct sum of indecomposable -modules, using the description of these modules given in Section 2.1, with the aim of eliminating all but one possibility.
First we use the fact that the decomposition of has to be compatible with the Jordan form of on (this can be read off from the relevant tables in [14]). In addition, it must be compatible with the known eigenvalues of on (as noted above, these are just the eigenvalues of on , which we can compute from the known action of on ). Note that if is an indecomposable summand of then the restriction of to is completely reducible, so we just need to identify the -composition factors of in order to compute the eigenvalues of on this summand. Often it is sufficient to compare the eigenvalues of on with the expected eigenvalues in (13), and we can also use our earlier calculations on the traces of elements of order and to obtain further restrictions on (see Section 2.2). With this approach in mind, the following lemma will be useful.
Lemma 2.20**.**
Let be an indecomposable -module of the form , or , where and . Then the eigenvalues of on are , and , respectively.
Proof.
First recall that has Jordan form , and on , and , respectively. The fixed point of on the simple module has highest weight , so the result is clear in this case. Similarly, so has eigenvalue on . Finally, suppose . The highest weight of is , so is one of the eigenvalues of on . To determine the second eigenvalue, it is helpful to view as the restriction to of the tilting module for the ambient algebraic group of type (see [28, Lemma 2.3]). On the latter module, has a fixed point of weight (the high weight), so the eigenvalue of is as required. ∎
Let us illustrate how Step 1 is carried out in the specific case .
Example 2.21**.**
Suppose and , so has Jordan form on (see [14, Table 9]). In particular, is projective and thus every indecomposable summand of is also projective. In terms of the notation introduced in Section 2.1, the possibilities for are as follows
[TABLE]
where and . If has an summand, then has an eigenvalue on , which contradicts (13), so we must have
[TABLE]
Since and has eigenvalues on (see Lemma 2.20), it follows that
[TABLE]
(see Table 3). Up to a re-ordering of summands, this immediately implies that
[TABLE]
Let be an involution. Since and (see Lemma 2.7 and Proposition 2.8), it follows that for all , whence and thus is the only possibility. We have now reduced to the case where the decomposition of is compatible with (see Table 2).
Step 2: Extension. Next observe that if has the decomposition given in Table 2 then the socle of has a simple summand . To complete the argument, we aim to show that is an -subalgebra of and its stabilizer in is an -type subgroup. We can do this in almost every case; the exceptions are the two special cases appearing in the statement of Theorem 1.
Let be a basis for , where is an eigenvector for with eigenvalue . We may assume that the action of on is given by the matrix
[TABLE]
with respect to this basis (that is, , etc.). If we define as above then is a Borel subgroup of and we can consider the opposite Borel subgroup of , where is also a regular unipotent element of order . With respect to the above basis, we may assume that acts on via the matrix
[TABLE]
If all these conditions are satisfied, then we will say that is a standard basis for .
With the aid of Magma [3] we can construct a matrix to represent the action of on with respect to our Chevalley basis . Let us illustrate this with an example.
Example 2.22**.**
For we proceed as follows in Magma:
G:=GroupOfLieType("G2",Rationals()); L:=LieAlgebra(G); e,f,h:=ChevalleyBasis(L); I1:=[1..6]; I2:=[1..2];
B:=[f[7-i] : i in I1] cat [e[i]*f[i] : i in I2] cat [e[i] : i in I1]; L:=ChangeBasis(L,B); B:=Basis(L); e:=[B[8+i] : i in I1]; f:=[B[7-i] : i in I1]; h:=[B[6+i]: i in I2];
ad:=AdjointRepresentation(L); y:=ad(e[1]+e[2]); A:=MatrixAlgebra(Rationals(),14); x:=Identity(A); y:=A!y; for i in [1..10] do x:=x+(1/Factorial(i))*y^i; end for; B:=MatrixAlgebra(GF(7),14); x:=B!x;
In this example, we are working with a Chevalley basis
[TABLE]
where spans the root space of the -th positive root, is in the root space of the corresponding negative root, and for , with respect to the following ordering
[TABLE]
of positive roots (note that this agrees with the ordering given by the Magma command PositiveRoots(G)). We adopt an analogous set-up in all cases.
Moreover, we can use Proposition 2.13(iv) to compute the eigenvalues and eigenvectors of (and thus ) on in terms of . For , it will be convenient to write for the -eigenspace of on (so for the elements in a standard basis of ).
Next we identify a basis of the -eigenspace in terms of , where (see Table 3). Since we can write
[TABLE]
for some , where only if . Similarly,
[TABLE]
Using Magma it is straightforward to compute bases for the relevant kernels; these computations can be done by hand, but it is much quicker and more efficient to use a machine.
Given these bases, say , and , we can write
[TABLE]
for and our goal is to determine these scalars. To do this, we can use the specified actions of and on to derive relations between the coefficients. Further relations can be determined by exploiting the fact that and are regular unipotent elements. For example, we observe that and
[TABLE]
where is the Lie bracket on , so . Since the regularity of implies that is abelian, it follows that is an abelian subalgebra of (for the latter equality, recall that ) and thus
[TABLE]
Proceeding in this way, our goal is to reduce to the case where is an -subalgebra, with and . Moreover, we want to find integers such that is an -triple over (that is, an -triple of in the notation of Section 2.3). Indeed, if we can do this, then Proposition 2.14 implies that the stabilizer of in is an -type subgroup and so we are in the generic situation described in part (i) of Theorem 1. In a few cases, we are unable to force , but by appealing to Proposition 2.15 we can still show that the same conclusion holds.
In the remaining cases where is not an -subalgebra, or the action of on is incompatible with , we will show that stabilizes a non-zero subalgebra of . More precisely, we will establish the following result, which reduces the proof of Theorem 1 to the handful of cases appearing in Table 4 (see Remark 1(a) for the conjugacy statement in part (i)).
Theorem 2.23** (Reduction Theorem).**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and set with Chevalley basis as in (11). Then one of the following holds:
- (i)
* is contained in an -type subgroup of and is uniquely determined up to -conjugacy;*
- (ii)
* stabilizes a non-zero subalgebra of and is one of the cases in Table 4.*
We will prove the Reduction Theorem in Sections 3–7, considering each possibility for in turn.
Step 3: Parabolic analysis. The final step in our proof of Theorem 1 concerns the cases arising in Theorem 2.23(ii), given in Table 4. In view of Proposition 2.18, we may assume that is contained in a proper parabolic subgroup of and we proceed by studying the possible embeddings of in such a subgroup. Take to be a minimal such parabolic and let be the quotient map. By identifying with , we may view as a subgroup of . Now we can show that , where is an -type subgroup of containing a regular unipotent element of (namely, ), so we can use [15, Tables 1–5] to study the composition factors of for each . In turn, this imposes restrictions on the decomposition of . But the possibilities for are listed in Table 4 and in this way we arrive at the two special cases in the statement of Theorem 1. See Section 8 for the details. (Notice that we adopt a similar approach in the proof of Theorem 2 below.)
Example 2.24**.**
To illustrate some of the above ideas, let us explain how we handle the case . Recall that in Example 2.21 we reduced to the situation where
[TABLE]
which is compatible with the decomposition of . By following the approach in Example 2.22, we use Magma to determine the action of on in terms of a Chevalley basis .
Let and let be a standard basis of as above. First consider . Now is -dimensional (indeed, by inspecting Table 3 we see that there is a unique which is congruent to modulo ), spanned by the sum of the simple root vectors, so we must have
[TABLE]
for some non-zero scalar . Similarly, is contained in the -dimensional space and by considering the relation we take
[TABLE]
Finally, is in the -dimensional space (note that since ) and it follows that
[TABLE]
where is the highest root. Note that since and .
By considering the action of on (see (14)) we quickly deduce that and . Finally, one checks that the condition in (16) yields , so setting we have
[TABLE]
and it is easy to see that and satisfy the relations
[TABLE]
and thus is an -subalgebra. If we set
[TABLE]
then is an -triple. Moreover, working mod , we have
[TABLE]
and thus is an -triple over (see the proof of [35, Proposition 2.4]). Since stabilizes , it is contained in an -type subgroup of by Proposition 2.14. This completes the proof of Theorem 1 for with .
We close this section by presenting a proof of Theorem 2.
Proof of Theorem 2. Let be the adjoint module for . Seeking a contradiction, suppose , where is a proper parabolic subgroup of with unipotent radical and Levi factor . We may as well assume that is minimal with respect to the containment of . In particular, if is the quotient map and we identify with , then is not contained in a proper parabolic subgroup of . Now is a regular unipotent element of (see [36, Lemma 2.6]). Writing , where each is a simple factor, let be the naturally defined projection map. Then contains a regular unipotent element of and does not lie in a proper parabolic subgroup of .
If is of classical type, we apply the main theorem of [29] to see that is contained in an -type subgroup of . On the other hand, if is of exceptional type, then is of type and is of type for . In this case, we apply Theorem 2.23 to conclude once again that is contained in an -type subgroup of for all relevant values of . In particular, in all cases we deduce that lies in an -type subgroup of .
Now the -composition factors of can be read off from the information in [15, Tables 1–5] and we can use this to determine the -composition factors of (to do this, note that we may set all in terms of the notation in [15, Tables 1–5]). Indeed, each composition factor of is an irreducible -module (the unipotent radical acts trivially on the -composition factors of ), so the decompositions of and have to be compatible. But the decomposition of is given in Table 2 and in this way we will reach a contradiction.
To see this, first observe that has at least one trivial composition factor on , coming from . By inspecting Table 2, this immediately implies that
[TABLE]
Suppose . From Table 2, the -composition factors of are as follows:
[TABLE]
By inspecting [15, Table 5], using the fact that has a unique trivial composition factor, we deduce that , or . However, in each of these cases we see that has an composition factor, which is incompatible with (19). The other two possibilities for can be eliminated in a similar fashion. For example, if then the composition factors of are
[TABLE]
By inspecting [15, Table 3], just considering trivial composition factors, we deduce that , or , but in each case we find that has two or more factors. This is a contradiction.
As mentioned above, the proof of Theorem 2.23 will be given in Sections 3–7, where we carry out Steps 1 and 2 (elimination and extension) for each group in turn. We handle Step 3 in Section 8, thus completing the proof of Theorem 1.
3. The case
We begin the proof of Theorem 1 by handling the case . As noted in Remark 1(c), the result in this case can be deduced from the proof of [30, Lemma 3.1] (it also follows from Kleidman’s classification of the maximal subgroups of in [13]).
Theorem 3.1**.**
Let be a simple algebraic group of type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of . Then is contained in an -type subgroup of .
Proof.
The Coxeter number of is , so we have . Let be the adjoint module for and fix a Chevalley basis for as in (11). We will use the notation introduced in Section 2.5. In particular, is a Borel subgroup of , where and
[TABLE]
are the eigenvalues of on , where . Let be the -eigenspace of on and recall from Section 2.3 that we may assume is obtained by exponentiating the regular nilpotent element (that is, we will assume ). According to [14, Table 2], the Jordan form of on is as follows:
[TABLE]
We will use the notation and for the projective indecomposable -modules defined in (3) and (4), respectively.
Case 1. is semisimple
First assume is semisimple and recall that has Jordan form on (for ). In view of (21), it follows that
[TABLE]
If then the above decomposition implies that is an eigenvalue of on , but this is not compatible with (20).
Now assume , so . As in Section 2.5, let be a standard basis for the summand , so and the action of on is given by the matrix in (14). Our goal is to show that is an -subalgebra with and . Furthermore, we seek integers so that is an -triple over , which will allow us to apply Proposition 2.14.
For we find that each space
[TABLE]
is -dimensional, which gives us
[TABLE]
for some non-zero scalars (in the expressions for and , the specific coefficients of the and will depend on the characteristic ; the coefficients presented here are for ). If we set then by considering the action of on we deduce that and . Now and satisfy the relations in (17), so we get an -triple as in (18). Here (for ) and thus is an -triple over (see the proof of [35, Proposition 2.4]). Finally, by applying Proposition 2.14, we conclude that is contained in an -type subgroup of .
Next assume . Once again and are -dimensional, but now is -dimensional, spanned by the vectors and (here we use the notation for with ). Therefore
[TABLE]
for some . By considering the action of on we deduce that and . Moreover, (16) implies that and by arguing as above, setting and using Proposition 2.14, we deduce that is contained in an -type subgroup of .
Now suppose . Here we have
[TABLE]
and by considering the action of on we deduce that , and . We may as well set , so
[TABLE]
for some . One now checks that the relations in (17) are satisfied (for all ), so is an -subalgebra. Moreover, if we take
[TABLE]
then is an -triple over and we can apply Proposition 2.15 (with and ). It follows that the stabilizer of in is an -type subgroup.
Case 2. ,
To complete the proof of the theorem we may assume that . Suppose and is a reducible indecomposable summand of . If then (see Corollary 2.4) and thus Lemma 2.1 implies that has a Jordan block of size on , but this is incompatible with (21). Now assume . Here (21) implies that has at least three composition factors (if there were only two, then Lemma 2.1 and Corollary 2.3 would imply that has Jordan form or on , which contradicts (21)). By Lemma 2.1, it follows that has Jordan form on with , so . By considering Theorem 2.2, it is easy to see that is the only possibility, so is projective and thus
[TABLE]
However, this implies that an involution has trace on (see Section 2.2), which is incompatible with Proposition 2.8. This is a contradiction.
Case 3. ,
Finally, let us assume . Let be a Sylow -subgroup of and observe that is projective. Then [1, Corollary 3, Section 9] implies that is projective and thus each indecomposable summand is also projective. Since the eigenvalues of on are , we deduce that or . In fact, by considering the trace of , we see that is the only option. This is compatible with the decomposition of with respect to an -type subgroup of containing a regular unipotent element (see Table 2).
Let be the summand in the socle of and let be a standard basis. The spaces and are -dimensional, whereas is -dimensional and we get
[TABLE]
for some . Set , so . By considering the action of on we deduce that . Moreover, (16) implies that and we deduce that is an -subalgebra and the relations in (17) are satisfied. As before, the desired result now follows by applying Proposition 2.14.
This completes the proof of Theorem 3.1. ∎
4. A reduction for
In this section our goal is to establish Theorem 2.23 when . The proof of Theorem 1 in this case will be completed in Section 8. Our main result is the following.
Theorem 4.1**.**
Let be a simple algebraic group of type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and set . Then one of the following holds:
- (i)
* is contained in an -type subgroup of ;*
- (ii)
, and stabilizes a non-zero subalgebra of .
Proof.
Here and we set up the standard notation as before. In particular,
[TABLE]
are the eigenvalues of on , where , and
[TABLE]
is the Jordan form of on (see [14, Table 4]). We may assume that is obtained by exponentiating the regular nilpotent element in , with respect to a Chevalley basis for as in (11). It will also be useful to note that is self-dual.
Case 1. is semisimple
If then (24) implies that
[TABLE]
but none of these decompositions are compatible with the eigenvalues of on given in (23). For example, if then the given decomposition implies that the relevant eigenvalues are , but this contradicts (23).
Now assume , so
[TABLE]
Let be the summand and let be a standard basis for as in Section 2.5, so (the -eigenspace of on ) and the action of and on is given by the matrices in (14) and (15), respectively, where is the opposite Borel subgroup of . If then the spaces in (22) are -dimensional and we get
[TABLE]
for some (in the expressions for and , the specific coefficients depend on the characteristic ; the ones given here are for ). If we set then we can use the action of on to deduce that and . Moreover, the relations in (17) are satisfied and it follows that is an -triple, where these elements are defined in (18). Now
[TABLE]
working mod (for ), so is an -triple over (see the proof of [35, Proposition 2.4]). By applying Proposition 2.14, we conclude that is contained in an -type subgroup of .
Now suppose . Here
[TABLE]
for some (we use the notation for with , and similarly for ). By considering the action of on we deduce that , and . Setting we get
[TABLE]
for some , and one can check that the relations in (17) are satisfied. In particular, is an -subalgebra of . Set
[TABLE]
and
[TABLE]
Then is an -triple over and by applying Proposition 2.15 (with and ) we deduce that the stabilizer of in is an -type subgroup.
Case 2. ,
For the remainder we may assume that . First assume . By arguing as in Case 2 in the proof of Theorem 3.1, it is straightforward to reduce to the case . For example, suppose and is a reducible indecomposable summand of . The Jordan form of on (see (24)) implies that has at least three composition factors and we can use Lemma 2.1 to see that has Jordan form on with , so . Using Theorem 2.2, we deduce that is the only option, so
[TABLE]
But this implies that an involution has trace [math] on , which is incompatible with Proposition 2.8.
Now assume . Suppose is a reducible non-projective indecomposable summand of . By combining Lemma 2.1 and Theorem 2.2 we deduce that has Jordan form or on , so there is a unique such summand (and the other summand is simple). However, this is incompatible with the self-duality of . For example, if has Jordan form on , then and Theorem 2.2 implies that
[TABLE]
(up to duality) so is not self-dual.
Therefore, we may assume that each indecomposable summand is either simple or projective, so the possibilities for are as follows:
[TABLE]
with . As in (23), the eigenvalues of on are
[TABLE]
Since has eigenvalues and on and , respectively (see Lemma 2.20), it follows that
[TABLE]
with . The case can be ruled out by considering the trace of ; hence and is compatible with the containment of in an -type subgroup of (see Table 2). We need to show that is contained in such a subgroup. To do this we can repeat the argument in Case 1 for (the details are entirely similar).
Case 3. ,
Now assume . Suppose is a reducible non-projective indecomposable summand of . It is easy to check that the Jordan form of on is either or , so there is a unique such summand. If has Jordan form on then Theorem 2.2 implies that (up to duality) where
[TABLE]
but this is incompatible with the self-duality of . Similarly, in the other case we have and
[TABLE]
with and . By self-duality, is the only option. But this implies that has trace [math] on , which contradicts Proposition 2.8.
It follows that each indecomposable summand of is either simple or projective. By arguing as above (the case ), using the fact that has eigenvalues on , we deduce that
[TABLE]
with . If then one can check that an element of order has trace on , so Proposition 2.8 implies that . Therefore, the action of is compatible with an -type subgroup of (see Table 2) and it remains to establish the desired containment.
As before, let be a standard basis of the summand in the decomposition of . In the usual manner we deduce that
[TABLE]
for some non-zero scalars . We may assume . Now is contained in , which is -dimensional, and we get
[TABLE]
Since the action of on is given by the matrix in (14) we deduce that and . Finally, the condition in (16), which is obtained by considering the action of on , implies that . It is easy to see that the relations in (17) are satisfied and we complete the argument in the usual manner, via Proposition 2.14.
Case 4. ,
Finally, let us assume that . Here is projective and thus each indecomposable summand is also projective. Since the eigenvalues of on are , we quickly deduce that is one of the following:
[TABLE]
Let be an element of order , where is -conjugate to a diagonal matrix and is a non-trivial -th root of unity. For each decomposition we can compute the eigenvalues of on and then compare the results with the list of eigenvalue multiplicities of all elements in of order (as noted in Remark 2.10, the latter can be computed using Litterick’s algorithm in [21]). For example, if then is conjugate to the diagonal matrix
[TABLE]
but one checks that no element in of order acts on with these eigenvalues. In this way, we deduce that is the only possibility.
Let be the summand in the socle of and let be a standard basis. The spaces and are -dimensional and we get
[TABLE]
for some . Finally, one checks that is -dimensional and we take
[TABLE]
In the usual manner, by considering the action of on , we get , , and . In addition, the condition in (16) yields the following system of equations:
[TABLE]
If then these equations imply that , so
[TABLE]
and by setting we can use Proposition 2.14 to show that is contained in an -type subgroup. On the other hand, if then we can set , so
[TABLE]
One checks that , so
[TABLE]
and we deduce that , hence
[TABLE]
It is now easy to check that is a subalgebra, which gives case (ii) in the statement of the theorem.
This completes the proof of Theorem 4.1. ∎
5. A reduction for
The following result, which we prove in this section, establishes Theorem 2.23 for groups of type .
Theorem 5.1**.**
Let be a simple adjoint algebraic group of type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and set . Then one of the following holds:
- (i)
* is contained in an -type subgroup of ;*
- (ii)
, is one of
[TABLE]
and stabilizes a non-zero subalgebra of .
Proof.
Here , is self-dual and
[TABLE]
are the eigenvalues of on , where (see Section 2.5). By inspecting [14, Table 6], we see that
[TABLE]
is the Jordan form of on . We adopt the notation introduced in Section 2.
Case 1. is semisimple
If then
[TABLE]
but not one of these decompositions is compatible with the eigenvalues of on (see (25)) so we may assume and
[TABLE]
Let be the summand and let be a standard basis for . If then one checks that each of the spaces in (22) are -dimensional and the result quickly follows via Proposition 2.14. For example, if then
[TABLE]
and by setting and considering the action of on (see (14)), we deduce that and . One now checks that is an -triple over (see the proof of [35, Proposition 2.4]) and by applying Proposition 2.14 we deduce that is contained in an -type subgroup of .
Now assume . Here and are -dimensional and we get
[TABLE]
where . Set . From the action of on we deduce that , and , so
[TABLE]
for some . If we take
[TABLE]
and
[TABLE]
then is an -triple over and using Proposition 2.15 we conclude that is contained in an -type subgroup of .
Case 2. ,
If then we can essentially repeat the argument in the proof of Theorem 4.1 (see the first paragraph in Case 2). Indeed, it is easy to reduce to the case where and
[TABLE]
but this is not compatible with (25).
Now assume . Suppose has a reducible non-projective indecomposable summand . By applying Lemma 2.1 and Theorem 2.2, we deduce that the Jordan form of on is one of the following:
[TABLE]
In particular, has a unique such summand. The structure of is described in Theorem 2.2 and it is easy to see that the existence of such a summand contradicts the self-duality of . For instance, suppose has Jordan form on . Then up to duality we have
[TABLE]
and thus is not self-dual. The other cases are very similar.
Therefore, we may assume that each indecomposable summand of is either simple or projective. By considering the eigenvalues of in (25), we deduce that
[TABLE]
with . If then we find that has trace on , which contradicts Proposition 2.8, hence is the only possibility. In the usual manner, we now construct a basis
[TABLE]
(with ) of the summand of . If we set and consider the action of on (see (14)) we deduce that and , and one checks that the condition in (16) gives . The result now follows in the usual manner via Proposition 2.14.
Case 4. ,
First assume that has a reducible indecomposable non-projective summand . In the usual way, by combining Lemma 2.1 and Theorem 2.2, we deduce that the Jordan form of on is one of the following:
[TABLE]
Suppose that has Jordan form on , so . By applying Theorem 2.2, using the self-duality of , we deduce that
[TABLE]
is the only possibility, but this is incompatible with the eigenvalues of on . We can rule out and by the self-duality of , so let us assume has Jordan form on . By self-duality it follows that
[TABLE]
and thus is one of the following:
[TABLE]
where and . However, it is clear that none of these decompositions are compatible with (25).
For the remainder, we may assume that each indecomposable summand of is either simple or projective. By considering the eigenvalues of , we deduce that
[TABLE]
with and . By computing the trace of and appealing to Proposition 2.8 (and also Remark 2.9), it follows that and is the only possibility. In particular, we have now reduced to the case where the decomposition of is compatible with containment in an -type subgroup of (see Table 2).
As before, let be the summand of and let be a standard basis of . The reader can check that
[TABLE]
with . Set . By considering the action of on we deduce that , and . The condition in (16) yields , so and thus
[TABLE]
for some . In addition, the relations in (17) are satisfied and is an -subalgebra of . Set
[TABLE]
and
[TABLE]
Then is an -triple over and by applying Proposition 2.15 (with and ) we conclude that is contained in an -type subgroup of .
Case 5. ,
Here (26) implies that is projective, so each indecomposable summand is also projective. In view of (25), we must have with and . In each case, the traces of and are and , respectively, so we need to work harder to eliminate some of these decompositions. Let be an element of order , where is -conjugate to a diagonal matrix and is a non-trivial -th root of unity. We can compute the eigenvalues of on and then compare with the eigenvalue multiplicities of all elements in of order , which we obtain using the algorithm in [21]. In this way, we deduce that is one of the following:
[TABLE]
Case 5(a). ,
Here is compatible with the containment of in an -type subgroup of (see Table 2). Let be the summand in the socle of and let be a standard basis. In the usual manner, we deduce that
[TABLE]
for some scalars . By considering the action of on , together with the condition in (16), we see that
[TABLE]
and either or . In the latter situation, we set and then check that the relations in (17) are satisfied – this allows us to apply Proposition 2.14 to conclude that is contained in an -type subgroup of . Now assume and set . Here one checks that , so since preserves the Lie bracket on . This yields , so
[TABLE]
We conclude that is an -invariant subalgebra of , as in part (ii) of the theorem.
Case 5(b). , or
Let be the summand in the socle of and let be a basis of with . We may assume that the actions of and on are given by the matrices
[TABLE]
respectively (in terms of this basis). One checks that is -dimensional, whereas the spaces
[TABLE]
are -dimensional, and
[TABLE]
have dimension and , respectively, and we get
[TABLE]
for some .
Set and consider the relations among the obtained from the action of on this basis. It is also helpful to note that is a regular unipotent element, so is abelian and we see that since . In this way, we deduce that
[TABLE]
Next one checks that , so and thus
[TABLE]
since preserves the Lie bracket. This yields . Similarly, and thus
[TABLE]
This relation implies that and it is now straightforward to check that is a subalgebra.
This completes the proof of Theorem 5.1. ∎
6. A reduction for
In this section we establish the following result, which proves Theorem 2.23 for groups of type .
Theorem 6.1**.**
Let be a simple adjoint algebraic group of type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and set . Then one of the following holds:
- (i)
* is contained in an -type subgroup of ;*
- (ii)
, is one of
[TABLE]
[TABLE]
and stabilizes a non-zero subalgebra of .
Proof.
Here we have and
[TABLE]
is the collection of eigenvalues of on , where . By [14, Table 8], the Jordan form of on is as follows:
[TABLE]
Note that is self-dual.
Case 1. is semisimple
If then the eigenvalues of on are incompatible with (29), so we may assume and thus
[TABLE]
in view of (30). Let be the summand and let be a standard basis for . In the usual manner, it is straightforward to show that is an appropriate -subalgebra and we can use Proposition 2.14 to show that (i) holds in the statement of the theorem. For example, if we get
[TABLE]
If we set , then by considering the action of on , we deduce that and . Furthermore, the relation in (16) implies that and we deduce that is an -triple over (see the proof of [35, Proposition 2.4]). Now apply Proposition 2.14.
Case 2. ,
If then a combination of Lemma 2.1 and Corollary 2.4 implies that has a Jordan block of size on , but this contradicts (30).
Next assume . In the usual way, by applying Lemma 2.1 and Theorem 2.2, and by appealing to the self-duality of , we can reduce to the case where each indecomposable summand of is either simple or projective. By considering the eigenvalues in (29), it follows that
[TABLE]
with . If then an involution has trace on , which contradicts Proposition 2.8. Therefore and it is entirely straightforward to show that the summand of is an appropriate -subalgebra. The result follows via Proposition 2.14 in the usual fashion.
A similar argument applies when . If has a reducible non-projective summand then the self-duality of implies that
[TABLE]
is the only possibility, where
[TABLE]
and . However, this implies that has trace on , which is a contradiction. Therefore, the indecomposable summands of are simple or projective, and by considering the eigenvalues in (29) we deduce that
[TABLE]
with . We can rule out by computing the trace of , so and we complete the argument as in the previous case.
Case 3. ,
As before, it is not difficult to reduce to the case where each indecomposable summand of is either simple or projective. By considering the eigenvalues in (29) we deduce that
[TABLE]
where , and . By computing the trace of we see that or , and we can rule out the first possibility by considering the trace of . This calculation with also implies that , so
[TABLE]
Let be the summand and fix a standard basis . By considering the spaces
[TABLE]
we deduce that
[TABLE]
Setting and using the action of on , we deduce that , and , so we have
[TABLE]
for some . One can check that the relations in (17) are satisfied, so is an -subalgebra of . Set
[TABLE]
[TABLE]
and
[TABLE]
Then is an -triple over and we can use Proposition 2.15 to deduce that is contained in an -type subgroup of .
Case 4. ,
Finally, let us assume so is projective and each indecomposable summand is also projective. By considering the eigenvalues in (29), it follows that
[TABLE]
where , , and . By computing the trace of we see that is one of the following:
[TABLE]
In all of these cases, has trace on , which is compatible with Proposition 2.8. If then there is an element of order with eigenvalues on , but one checks that there are no elements in that act on in this way (for example, see [7, Table 6]), so this possibility is ruled out.
If is one of
[TABLE]
[TABLE]
then stabilizes the -dimensional subalgebra of spanned by the vector
[TABLE]
Indeed, stabilizes , which is spanned by a vector in . But one checks that so we are in case (ii) in the statement of the theorem.
Finally, suppose , which is compatible with the containment of in an -type subgroup of (see Table 2). Let be the summand in the socle of and let be a standard basis. In the usual way we obtain
[TABLE]
and we may assume . By considering the action of on , together with the condition in (16), we deduce that , , and , so we have
[TABLE]
for some . Set
[TABLE]
[TABLE]
and
[TABLE]
Then is an -triple over , but we cannot directly apply Proposition 2.15. However, a minor modification of the argument in the proof of that proposition will work.
First observe that , and (in terms of the notation used in the proof of Proposition 2.15). Setting , we see that
[TABLE]
is an -triple in for all choices of . Put and note that
[TABLE]
(for the final equality, note that all higher degree terms are zero since the maximum -weight on is ). Now calculating (in ), we have
[TABLE]
and passing to , setting , we deduce that
[TABLE]
Therefore and by comparing -weights we deduce that and . Finally, this implies that
[TABLE]
and we can now conclude as in the proof of Proposition 2.15. In particular, is contained in an -type subgroup of .
This completes the proof of Theorem 6.1. ∎
7. A reduction for
In this section we complete the proof of the Reduction Theorem (see Theorem 2.23). Our main result is the following:
Theorem 7.1**.**
Let be a simple algebraic group of type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and set . Then one of the following holds:
- (i)
* is contained in an -type subgroup of ;*
- (ii)
, and stabilizes a non-zero subalgebra of .
Proof.
First note that . In fact, we may assume since the case was handled in Section 2 (see Examples 2.21 and 2.24). Recall that
[TABLE]
is the collection of eigenvalues of on and note that is self-dual. The Jordan form of on is as follows:
[TABLE]
(see [14, Table 9]).
Case 1. is semisimple
By considering the eigenvalues in (31) we deduce that and
[TABLE]
Let be the summand and let be a standard basis. If then it is straightforward to show that is an appropriate -subalgebra and the result follows by applying Proposition 2.14 (note that if then is -dimensional, but this does not cause any special difficulties). Now assume . Here and are both -dimensional and we get
[TABLE]
Set and consider the action of on (see (14)). We deduce that , and , so
[TABLE]
for some . Set
[TABLE]
and
[TABLE]
Then is an -triple over (see the proof of [35, Proposition 2.4]) and by applying Proposition 2.15 (with and ) we deduce that is contained in an -type subgroup of .
Case 2. ,
If then the dimension of each indecomposable summand of is at least , which implies that the Jordan form of has a block of size . This is a contradiction.
Next assume . Suppose is a reducible indecomposable non-projective summand of , so (see Corollary 2.4). In view of (32) and Lemma 2.1, we deduce that has Jordan form on for some odd integer between and . But this implies that is even, so Corollary 2.3 implies that has at least four composition factors and thus (again, by Corollary 2.4). This is a contradiction. Therefore, we may assume that each indecomposable summand of is either simple or projective. Clearly,
[TABLE]
is the only possibility. However, this implies that has trace on , which contradicts Proposition 2.8.
Now assume . As in the previous case, by applying Lemma 2.1 and Theorem 2.2, and by appealing to the self-duality of , it is straightforward to reduce to the case where the indecomposable summands of are either simple or projective. Moreover, by considering the eigenvalues in (31), we deduce that
[TABLE]
with . By computing the trace of , it follows that . It is now entirely straightforward to show that the summand of is an appropriate -subalgebra and the result follows via Proposition 2.14.
Case 3. ,
As in the previous case, we can quickly reduce to the situation where each indecomposable summand of is simple or projective, in which case
[TABLE]
with and . By computing the trace of we deduce that and , in which case is compatible with the containment of in an -type subgroup of (see Table 2).
As usual, let be the summand of and let be a standard basis for . We get
[TABLE]
We may set . By considering the action of on this basis we deduce that , and , so
[TABLE]
for some . One now checks that the relations in (17) are satisfied and thus is an -subalgebra of . Set
[TABLE]
and
[TABLE]
Then is an -triple over (see the proof of [35, Proposition 2.4]) and we can use Proposition 2.15 to conclude that is contained in an -type subgroup of .
Case 4. ,
By arguing in the usual manner, it is straightforward to reduce to the case where each indecomposable summand of is either simple or projective. By considering the eigenvalues in (31), we deduce that
[TABLE]
with and . By computing the trace of , we see that is the only option, in which case is compatible with the desired containment of in an -type subgroup of . As usual, we now construct the summand of in terms of a standard basis ; it is easy to show that is an appropriate -subalgebra and we can conclude by applying Proposition 2.14.
Case 5. ,
First assume that has a reducible indecomposable non-projective summand . In the usual way, we deduce that the Jordan form of on is one of the following:
[TABLE]
If the Jordan form is either or then there is a unique such summand. Moreover, has an odd number of composition factors and it is easy to see that this is incompatible with the self-duality of . Similar reasoning rules out the cases where has Jordan form . Finally, suppose has Jordan form or . Here the self-duality of implies that
[TABLE]
or
[TABLE]
respectively. However, the existence of such a summand would mean that is an eigenvalue of on , which is not the case (see (31)). Therefore, we conclude that every indecomposable summand of is either simple or projective. More precisely, in view of (31), it follows that
[TABLE]
with and . By computing the trace of we deduce that , in which case is compatible with the containment of in an -type subgroup.
Let be the summand of and let be a standard basis. In the usual manner we deduce that
[TABLE]
Set . By considering the action of on this basis we get and . Finally, one can check that the condition in (16) implies that and now the desired result follows from Proposition 2.14.
To complete the proof of the theorem, we may assume that (recall that the case was handled earlier in Examples 2.21 and 2.24).
Case 6. ,
As usual, let us first assume that has a reducible indecomposable non-projective summand . By applying Lemma 2.1 and Theorem 2.2, we deduce that the Jordan form of on is one of the following:
[TABLE]
In fact, the self-duality of implies that is the only possibility, with
[TABLE]
But if this is a summand of then is an eigenvalue of on , contradicting (31). Therefore, we have reduced to the case where each indecomposable summand of is simple or projective. Again, by considering (31) we deduce that
[TABLE]
with , and .
We claim that , in which case the decomposition of is compatible with the containment of in an subgroup of . One can check that all of the eight decompositions above are compatible with the trace of and , so we consider the traces of elements of larger order. Let be an element of order . In each case it is straightforward to compute the eigenvalues of on . Using Litterick’s algorithm in [21], we can compute the eigenvalues on of every element in of order and in this way we deduce that as claimed.
Let be the summand of with standard basis . The spaces
[TABLE]
have respective dimensions , and , which gives
[TABLE]
By considering the action of on this basis, we deduce that , , and . The condition in (16) yields the equations
[TABLE]
If then these equations imply that , so we can set and then apply Proposition 2.14 to show that is contained in an -type subgroup. On the other hand, if then we may assume , so
[TABLE]
It is straightforward to check that is a subalgebra and this puts us in case (ii) of the theorem.
This completes the proof of Theorem 7.1. ∎
8. Proof of Theorem 1
In this final section we complete the proof of Theorem 1. In view of Theorem 3.1, we may assume that is of type , , or . Moreover, by our work in Sections 4–7, it remains to handle the cases appearing in Table 4. In each of these cases, stabilizes a non-zero subalgebra of and by applying Proposition 2.18 we can assume that is contained in a proper parabolic subgroup of with unipotent radical and Levi factor . The following result, when combined with Theorem 2, completes the proof of Theorem 1. (Recall that Craven [9] has constructed a subgroup satisfying the conditions in parts (ii) and (iii) of Theorem 1, and he has established its uniqueness up to conjugacy; see Remark 1(b).)
Theorem 8.1**.**
Let be a simple exceptional algebraic group of adjoint type over an algebraically closed field of characteristic . Let be a subgroup of containing a regular unipotent element of and let be the adjoint module. If is contained in a proper parabolic subgroup of , then either
- (i)
, , and ; or
- (ii)
, , and .
Proof.
We may assume that is minimal with respect to containing . Let be the quotient map and identify with . By arguing as in the first paragraph in the proof of Theorem 2 (see the end of Section 2), we deduce that is contained in an -type subgroup of . In addition, Theorem 2 implies that is not contained in an -type subgroup of , so must be one of the cases in Table 4. As noted in the proof of Theorem 2, the composition factors of can be read off from [15, Tables 1–5] and this imposes restrictions on the composition factors of . By considering each possibility for in turn, comparing composition factors with Table 4, we will show that the cases labelled (i) and (ii) in the statement of the theorem are the only compatible options.
First assume , so the composition factors of are , , and . By inspecting [15, Table 2] it is easy to see that there is no compatible Levi subgroup . Similarly, if then the composition factors of are given in (19) and thus we can eliminate this case by repeating the argument in the proof of Theorem 2.
Next suppose . The three possibilities for (and their composition factors) are as follows:
[TABLE]
In all three cases, we see that has at most two trivial composition factors, so [15, Table 3] implies that
[TABLE]
If then has five or more factors, which is incompatible with all three possibilities for . Similarly, if then there are too many factors, and we can rule out because we would get composition factors, which is absurd. Finally, suppose . Since the Weyl module has an composition factor, we see that has four such factors and thus
[TABLE]
is the only option.
Finally, let us assume . The three possibilities for are as follows:
[TABLE]
By inspecting [15, Table 4], counting the number of trivial composition factors, we quickly reduce to a small number of possibilities for . By considering non-trivial composition factors, it is straightforward to reduce further to the case . For example, we can rule out because there would be too many factors. Similarly, is out because we would have an and at least three factors, which is not compatible with any of the three possibilities above. We can rule out because it would imply that has an factor. Finally, suppose . Here has at least three and composition factors, so
[TABLE]
is the only possibility. ∎
Acknowledgements
Testerman was supported by the Fonds National Suisse de la Recherche Scientifique grants and . Burness thanks the Section de Mathématiques and the Centre Interfacultaire Bernoulli at EPFL for their generous hospitality. It is a pleasure to thank David Craven and Jacques Thévenaz for many useful discussions. We also thank Bob Guralnick, Gunter Malle and Iulian Simion for helpful comments on an earlier draft of this paper. Finally, we thank an anonymous referee for carefully reading the paper and for making several suggestions that have improved both the accuracy of the paper and the clarity of the exposition.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] J.L. Alperin, Local Representation Theory , Cambridge Stud. Adv. Math., vol. 11, Cambridge Univ. Press, 1986.
- 2[2] A. Borel and J. Tits, Éléments unipotents et sous-groupes paraboliques de groupes réductifs. I , Invent. Math. 12 (1971), 95–104.
- 3[3] W. Bosma, J. Cannon and C. Playoust, The Magma algebra system I: The user language , J. Symbolic Comput. 24 (1997), 235–265.
- 4[4] N. Bourbaki, Groupes et algebrès de Lie (Chapitres 4, 5 et 6) , Hermann, Paris, 1968.
- 5[5] R.W. Carter, Simple groups of Lie type , John Wiley and Sons, London, 1972.
- 6[6] R.W. Carter, Finite Groups of Lie Type: Conjugacy Classes and Complex Characters , John Wiley and Sons, London, 1985.
- 7[7] A.M. Cohen and R.L. Griess, On finite subgroups of the complex Lie group of type E 8 subscript 𝐸 8 E_{8} , Proc. Sympos. Pure Math. 47 (1987), 367–405.
- 8[8] B.N. Cooperstein, Maximal subgroups of G 2 ( 2 n ) subscript 𝐺 2 superscript 2 𝑛 G_{2}(2^{n}) , J. Algebra 70 (1981), 23–36.
