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Elementary abelian subgroups: from algebraic groups to finite groups

Jianbei An J. An: Department of Mathematics, University of Auckland, Auckland, New Zealand [email protected] Heiko Dietrich H. Dietrich: School of Mathematics, Monash University, Australia [email protected]  and  Alastair Litterick A. J. Litterick: School of Mathematics, Statistics and Actuarial Science, University of Essex, Wivenhoe Park, Colchester, Essex CO4 3SQ, England [email protected]
Abstract.

We describe a new approach for classifying conjugacy classes of elementary abelian subgroups in simple algebraic groups over an algebraically closed field, and understanding the normaliser and centraliser structure of these. For toral subgroups, we give an effective classification algorithm. For non-toral elementary abelian subgroups, we focus on algebraic groups of exceptional type with a view to future applications, and in this case we provide tables explicitly describing the subgroups and their local structure. We then describe how to transfer results to the corresponding finite groups of Lie type using the Lang-Steinberg Theorem; this will be used in forthcoming work to complete the classification of elementary abelian pp-subgroups for torsion primes pp in finite groups of exceptional Lie type. Such classification results are important for determining the maximal pp-local subgroups and pp-radical subgroups, both of which play a crucial role in modular representation theory.

2020 Mathematics Subject Classification:
Primary 20G07; Secondary 20G41, 20-08, 20D06, 22E40
The first author was supported by the Marsden Fund (of New Zealand), via award numbers UOA 1626 and UOA 2030. The second author thanks Jianbei An and Eamonn O’Brien for the hospitality during various invited research visits to the University of Auckland. The third author acknowledges support from a Humboldt Fellowship for Postdoctoral Researchers from the Alexander von Humboldt Foundation, Germany. The second and third author would like to thank the Isaac Newton Institute for Mathematical Sciences for support and hospitality during the programme “Groups, representations and applications: new perspectives” when work on this paper was undertaken. This work was supported by EPSRC Grant Number EP/R014604/1. The authors thank Meizheng Fu for a careful reading of the paper.

1. Introduction

Many open conjectures in representation theory, like the McKay, Dade, and Alperin Weight conjectures, have reductions to finite quasi-simple groups. For example, Navarro & Tiep [35] have shown that the Alperin Weight Conjecture is true for every finite group if every finite simple group satisfies a stronger condition, namely, AWC goodness. (For another example, see the recent work of Feng, Li & Zhang [19].) Verifying this latter property requires a detailed study of the finite simple groups and their covering groups. An important role in this study is played by so-called pp-radical subgroups and their pp-local structure—that is, subgroups RGR\leq G which satisfy R=Op(NG(R))R=O_{p}(N_{G}(R)), the largest normal pp-subgroup of the normaliser NG(R)N_{G}(R)—together with their normalisers NG(R)N_{G}(R) and centralisers CG(R)C_{G}(R). The recent articles of Malle & Kessar, e.g. [27], give an excellent survey of the current state of these conjectures and the role of pp-local structure. In fact, radical subgroups are relevant in many areas of modular representation theory: for instance, defect groups of blocks are radical, the subgroup RR of a weight (R,φ)(R,\varphi) is radical, and the first nontrivial subgroup in any radical chain is radical. If the radical subgroups of GG are known, then the essential rank of the Frobenius category D(G)\mathcal{F}_{D}(G) (DGD\leq G a Sylow subgroup) can be determined, cf. [2]. Radical subgroups are also used in the study of so-called pp-local geometries, cf. [28]. The classification of radical subgroups therefore is an important open problem; classifications are known for the symmetric, classical, and sporadic groups, as well as for some exceptional groups of Lie type, see [6] and the references therein.

One approach to classify pp-radical subgroups of a finite group GG is via its pp-local subgroups: A subgroup MGM\leq G is pp-local if it is the normaliser of a nontrivial pp-subgroup of GG. It is maximal pp-local if MM is maximal with respect to inclusion among all pp-local subgroups of GG. It is local maximal if it is pp-local for some prime pp and maximal among all subgroups of GG. If GG has a nontrivial normal pp-subgroup, then the only maximal pp-local subgroup is GG itself. Following the notation of previous works, we say M<GM<G is maximal-proper pp-local if MM is pp-local and maximal with respect to inclusion among all proper subgroups of GG that are pp-local. Thus if Op(G)=1O_{p}(G)=1 then the maximal-proper pp-local subgroups are exactly the maximal pp-local subgroups. Now, if RGR\leq G is pp-radical with Op(G)RO_{p}(G)\neq R, then NG(R)N_{G}(R) is pp-local and NG(R)NG(C)N_{G}(R)\leq N_{G}(C) for every characteristic subgroup CRC\leq R. In particular, NG(R)N_{G}(R) is contained in some maximal-proper pp-local MGM\leq G, so that NG(R)=NM(R)N_{G}(R)=N_{M}(R) and RR is pp-radical in MM. This shows that every radical pp-subgroup RR of GG with Op(G)RO_{p}(G)\neq R is radical in some maximal-proper pp-local subgroup M=NG(R)M=N_{G}(R) of GG. Since NG(R)NG(Ω1(Z(R)))N_{G}(R)\leq N_{G}(\Omega_{1}(Z(R))), one can show that every maximal-proper pp-local subgroup can be realised as the normaliser of an elementary abelian pp-subgroup. This approach has been used successfully in recent work [3, 4, 5, 6, 9, 10], leading to various classifications of pp-local and pp-radical subgroups in finite exceptional groups of Lie type. Similar to pp-radical groups, pp-local groups also play an important role in group theory. For example, large parts of the classification of the finite simple groups are based on the analysis of pp-local subgroups; one reason for this is that the fusion of pp-elements is controlled by normalisers of pp-subgroups, by the Alperin-(Goldschmidt) Fusion Theorem. We note that Cohen et al. [16] classified local maximal subgroups of exceptional groups of Lie type. However, not every maximal-proper pp-local subgroup is local maximal, and the details obtained in the classification of maximal-proper pp-local subgroups have proved useful for the classification of radical subgroups.

All of this highlights the importance of knowing the elementary abelian pp-subgroups of a finite group of Lie type; Griess [22, Section 1] lists more references supporting this. With the knowledge of the elementary abelian subgroups, one can attempt a classification of the maximal-proper pp-local and pp-radical subgroups. Recent efforts in this direction have focused directly on the finite groups involved (see [3, 4, 6, 9, 10] for groups of type F4F_{4}, E6E_{6}, E7E_{7}). In contrast, this paper takes an alternative approach beginning with an ambient algebraic group over an algebraically closed field. In this case, the rich geometric and Lie-theoretic structure of the group drastically simplifies many arguments, and indeed there are a number of existing results in this case [11, 22, 24, 41] which we will build upon here. Supposing one has complete subgroup structure information for a given algebraic group in positive characteristic, the Lang-Steinberg Theorem (cf. [32, §21.2]) then gives a powerful technique for transferring results to the corresponding finite groups of Lie type. This both streamlines arguments, and avoids some of the lengthy ad-hoc calculations required in previous papers.

We note that the results of this paper have already been used successfully in [5, 6] to classify the maximal 33-local and 33-radical subgroups in the finite groups of type E6E_{6}. It is also used in [8] for work on Donovan’s conjecture for blocks with extra-special defect groups p+1+2p_{+}^{1+2}, in [1] to classify weight subgroups of quasi-isolated 22-blocks of F4(q)F_{4}(q), and in the (ongoing) PhD thesis of Fu to classify elementary abelian subgroups in finite classical groups. In forthcoming work, we apply the results of this paper to classify the elementary abelian pp-subgroups in the finite exceptional groups of Lie type for small (torsion) primes. In particular, our results are also a significant step toward a classification of the maximal-proper pp-local subgroups in the finite groups of Lie type; this research will be published in a separate paper.

1.1. Main results and structure of the paper

Let pp be a prime and let GG be a simple algebraic group over an algebraically closed field of characteristic 0\ell\geq 0. If >0\ell>0, then we choose a Steinberg endomorphism FF of GG, with corresponding fixed-point subgroup GFG^{F}, a finite group of Lie type. If =p\ell=p, then the pp-radical subgroups of GFG^{F} are known by the Borel–Tits Theorem [21, Corollary 3.1.5], hence we assume throughout that p\ell\neq p. Thus each elementary abelian pp-subgroup of GG consists of semisimple elements, and therefore normalises a conjugate of a fixed maximal torus TGT\leq G. Our strategy is to consider separately the case of toral subgroups (those with a conjugate contained in TT) and non-toral subgroups (those which are not toral). While we consider the toral elementary subgroups for all simple algebraic groups, we restrict ourselves to exceptional groups for the non-toral ones; classification of non-toral elementary abelian groups in the classical case is more difficult (and is sometimes related to the classification of certain codes, see [22, Table 1]). Our main results are the following:

  • (1)

    A constructive method to classify the toral elementary abelian pp-subgroups (up to conjugacy) in a simple algebraic group GG and to determine information on their local structure, see Section 5. Our method translates to a practical algorithm that we have implemented for the computer algebra system Magma [13]; our implementation is available under the link provided in [7].

  • (2)

    A complete classification of the non-toral elementary abelian pp-subgroups (up to conjugacy) in an exceptional simple algebraic group GG and their local structure, see Proposition 6.1 for odd pp and Proposition 6.3 for p=2p=2.

  • (3)

    A description of how (1) and (2) can be used to classify the elementary abelian pp-subgroups (up to conjugacy) and their local structure in the finite groups GFG^{F}, see Section 4.

Remark 1.1.

In fact, our method for classifying subgroups in (1) and (2) works for any finite subgroup of order coprime to the characteristic \ell, and if the subgroups are moreover abelian, then the arguments relating to local structure also generalise. However, our results on torality depend implicitly on the fact that the subgroup in question is an abelian pp-group; for this reason and the reasons above, we keep our focus on the elementary abelian case.

First consider toral subgroups. For a maximal torus TT of GG, it is well known that the Weyl group NG(T)/TN_{G}(T)/T controls conjugacy and determines the normaliser structure of subgroups of TT. By viewing GG as the group of points of a suitable group scheme, it follows that the classification of toral elementary abelian pp-subgroups of GG is independent of the characteristic \ell as long as p\ell\neq p, which we assume throughout. Importantly, this shows that all of these calculations can be performed in a suitable finite group of Lie type, which gives rise to a practical computational approach toward a classification. We give full details in Section 5.

Turning to non-toral elementary abelian subgroups of an exceptional simple algebraic group in Section 6, the number of classes of such subgroups is bounded by an absolute constant, and in many cases these have been described elsewhere in the literature: For example, the maximal non-toral elementary abelian subgroups in complex groups are described by Griess [22]. Complete information on non-toral subgroups for p2p\neq 2 in groups over \mathbb{C} is given by Andersen et al. [11]. For p=2p=2, much information is provided by Yu [41] for adjoint compact groups. Again, all these results carry over into any characteristic different from pp. We present explicit tables (including new information on the local structure) and we use the opportunity to correct some typographic errors in the ancillary data of [41].

Assuming >0\ell>0, and using knowledge of the elementary abelian subgroups and their local structure in GG, in Section 4 we use a consequence of the Lang-Steinberg Theorem to see how the GG-classes of subgroups split into subgroups of the finite groups GFG^{F}. If some GG-conjugate of an elementary abelian subgroup EE lies in GFG^{F}, then the GFG^{F}-subgroup classes arising from EE correspond to FF-classes in NG(E)/CG(E)N_{G}(E)/C_{G}(E)^{\circ} of elements contained in CG(E)/CG(E)C_{G}(E)/C_{G}(E)^{\circ}, and these are known by our previous calculations. The normaliser and centraliser structure also follow in short order.

In Appendices A and B we give various ancillary data which we computed (or re-computed) in the course of proving our results for non-toral subgroups, in particular, for p=2p=2 and types E7E_{7} and E8E_{8}.

2. Notation

Throughout, unless stated otherwise, GG is a simple algebraic group, defined over an algebraically closed field KK of characteristic 0\ell\geq 0. When discussing elementary abelian pp-groups, we always assume pp\neq\ell, restating this assumption when necessary. We treat GG as a Zariski-closed subgroup of some general linear group over the algebraically closed field, except in Section 3.1 where we briefly mention the scheme-theoretic background necessary to transfer results between groups over fields of different characteristics. We add subscripts “sc” and “ad” to denote the simply-connected and adjoint group, respectively, of a given type.

For qq a prime power, we denote by 𝔽q\mathbb{F}_{q} the finite field with qq elements. We denote by TT a fixed maximal torus of GG, and define the Weyl group of GG as W=NG(T)/TW=N_{G}(T)/T; this does not depend on the choice of TT since all maximal tori in a linear algebraic group are conjugate [32, Corollary 6.5]. Recall that GG has an associated root datum, consisting of a root system Φ\Phi, dual root system Φ\Phi^{\vee}, character lattice X=Hom(T,K)ΦX=\operatorname{Hom}(T,K^{\ast})\supseteq\mathbb{Z}\Phi and co-character lattice Y=Hom(K,T)ΦY=\operatorname{Hom}(K^{\ast},T)\supseteq\mathbb{Z}\Phi^{\vee}, with a natural pairing ,:X×Y\left<-,-\right>\colon X\times Y\to\mathbb{Z}. There are natural notions of homomorphism and isomorphism of root data, and GG is determined up to isomorphism by its root datum and the field KK, see [25, II.1.13].

We follow the convention of Malle and Testermann [32, Section 21.2] and call an endomorphism F:GGF\colon G\to G of a linear algebraic group GG a Steinberg morphism if some power FmF^{m} is a Frobenius morphism with respect to some 𝔽q\mathbb{F}_{q}-structure, that is, FmF^{m} is induced by the qq-power map KKK\to K. A Steinberg morphism is an automorphism of abstract groups, but not necessarily of algebraic groups. As usual, if XX is a set and FF is a function XXX\to X, then we denote by XFX^{F} the fixed-point set of FF. If FF is a Steinberg morphism of a linear algebraic group with FmF^{m} a Frobenius morphism, then GFGFmG^{F}\leq G^{F^{m}} are both finite groups. We note that this implies FF is a Steinberg morphism as defined in Gorenstein et al. [21, Definition 1.15.1]. Lastly, we mention a celebrated result of Steinberg which shows that if GG is simple (the case of most interest here), then every non-trivial endomorphism of GG is either an automorphism of algebraic groups or a Steinberg morphism, and the latter occurs if and only if GFG^{F} is finite, see [32, Theorem 21.5].

For an algebraic group HH, we denote by HH^{\circ} the connected component of the identity element. If XX is a finite group then Op(X)O_{p}(X) denotes the largest normal pp-subgroup of XX, and if PP is a pp-group, then Ωk(P)\Omega_{k}(P), with k1k\geq 1 an integer, denotes the subgroup generated by elements of order dividing pkp^{k}.

Let A,BA,B be groups and l,n,ml,n,m be positive integers. Let pp be a prime. We denote by A×BA\times B the direct product of AA and BB. We sometimes write mm for the cyclic group of size mm, and we denote by AnA^{n} the direct product of nn copies of AA. This leads to an ambiguity if m=pnm=p^{n} is a prime power; we avoid this by writing pnp^{n} only for the direct product of groups of order pp, and mm for the cyclic group of order mm. An extension, split extension, and central extension of AA by BB are respectively denoted A.BA.B, A:BA{:}B, and ABA\circ B; here AA is the normal subgroup. We read A.B.CA.B.C as (A.B).C(A.B).C, and similarly for other products of groups. For group elements g,hAg,h\in A we denote conjugation as usual by hg=ghg1{}^{g}h=ghg^{-1} and hg=g1hgh^{g}=g^{-1}hg. The notation p1+2np^{1+2n} denotes an extraspecial group; there are two isomorphism types of these, which are denoted by p+1+2np_{+}^{1+2n} and p1+2np_{-}^{1+2n}. The alternating and symmetric group on nn points are denoted by Altn\operatorname{Alt}_{n} and Symn\operatorname{Sym}_{n}, respectively. The dihedral and generalised quaternion group of order nn are Dihn{\rm Dih}_{n} and QnQ_{n}. We write GLn(q)\operatorname{GL}_{n}(q) for the general linear group of degree nn over the field with qq elements, and SLn(q)\operatorname{SL}_{n}(q), SUn(q)\operatorname{SU}_{n}(q), Spn(q)\operatorname{Sp}_{n}(q), and On±(q)\operatorname{O}^{\pm}_{n}(q) for the classical groups (special linear, unitary, symplectic, and orthogonal group). Other notation is introduced at the appropriate places.

3. Preliminaries

3.1. Independence from the characteristic

The following result is of vital importance for establishing our main results. In the present form this is due to Larsen [23, Appendix A], but see also [11, p. 137], [17, Section 3], [22, Appendix A], and [20]. It tells us that the classification of elementary abelian pp-subgroups of GG is independent of the defining characteristic \ell, as long as it is different from pp; in particular, it shows that the classification of elementary abelian pp-subgroups of a semisimple algebraic group G(K)G(K) coincides with that of the corresponding complex Lie group G()G(\mathbb{C}). The proof makes use of deep algebraic geometry, interpreting GG as a group scheme over a ring of Witt vectors, which is an integral domain of characteristic 0 that maps onto an algebraically closed field of positive characteristic.

Proposition 3.1 ([23, Theorem 1.22]).

Let \ell be a prime number and GG a semisimple split group scheme; let XX be a finite group of order coprime to \ell. For any algebraically closed fields K0K_{0} and KK_{\ell} of characteristic 0 and \ell, respectively, the sets Hom(X,G(K0))/G(K0)\operatorname{Hom}(X,G(K_{0}))/G(K_{0}) and Hom(X,G(K))/G(K)\operatorname{Hom}(X,G(K_{\ell}))/G(K_{\ell}) have the same cardinality, where the quotients are taken with respect to the natural conjugation action of the groups on the homomorphism sets. Furthermore, the process of reduction modulo \ell induces a bijection.

The ‘process of reduction modulo \ell’ here entails showing that every finite subgroup of G(K0)G(K_{0}) has a conjugate contained in G(R)G(R), where RR is a suitable ring of Witt vectors that maps onto an algebraically closed subfield of KK_{\ell}, and then considering the induced map G(R)G(K)G(R)\to G(K_{\ell}); we refer to [23, Appendix A] and [20] for more details.

Recall, for instance from [11, Proposition 8.4], that a complex algebraic group G=G()G=G(\mathbb{C}) has a maximal compact subgroup in the Hausdorff topology, say HH, which is unique up to conjugacy and strongly controls fusion: if Ug=VU^{g}=V for subsets U,VHU,V\subseteq H and gGg\in G, then there is some hHh\in H such that ug=uhu^{g}=u^{h} for all uUu\in U. In particular, if Ug=UU^{g}=U, then gCG(U)NH(U)g\in C_{G}(U)N_{H}(U), so NG(U)=CG(U)NH(U)N_{G}(U)=C_{G}(U)N_{H}(U). Moreover, if UGU\leq G is a finite subgroup, then NG(U)/CG(U)N_{G}(U)/C_{G}(U) embeds into the (finite) automorphism group Aut(U)\operatorname{Aut}(U), and since CG(U)C_{G}(U)^{\circ} has finite index in CG(U)C_{G}(U), it has finite index in NG(U)N_{G}(U); thus, we have NG(U)=CG(U)N_{G}(U)^{\circ}=C_{G}(U)^{\circ}, and therefore NG(U)/NG(U)=NH(U)CG(U)/CG(U)N_{G}(U)/N_{G}(U)^{\circ}=N_{H}(U)C_{G}(U)/C_{G}(U)^{\circ}. Based on all this, the next lemma shows that we can view the pp-local structure of GG inside HH.

Lemma 3.2.

Let GG be a reductive complex algebraic group with a maximal compact subgroup HH, and let EHE\leq H be elementary abelian. Then the following hold:

  • (a)

    The inclusion HGH\hookrightarrow G induces a bijection on conjugacy classes of elementary abelian subgroups of GG.

  • (b)

    The group CG(E)HC_{G}(E)^{\circ}\cap H is a maximal compact subgroup of CG(E)C_{G}(E)^{\circ}, with the same root datum.

  • (c)

    We have

    NH(E)\displaystyle N_{H}(E) =(HNG(E)).(NG(E)/NG(E)), and\displaystyle=(H\cap N_{G}(E)^{\circ}).(N_{G}(E)/N_{G}(E)^{\circ})\text{, and}
    CH(E)\displaystyle C_{H}(E) =(HCG(E)).(CG(E)/CG(E)).\displaystyle=(H\cap C_{G}(E)^{\circ}).(C_{G}(E)/C_{G}(E)^{\circ}).
Proof.

By uniqueness of HH, each compact subgroup of GG has a GG-conjugate contained in HH. Uniqueness of this GG-conjugate up to HH-conjugacy follows since HH strongly controls fusion in GG; this proves (a). Next, by [11, Proposition 8.4(3)] the group CH(E)=HCG(E)C_{H}(E)=H\cap C_{G}(E) is a maximal compact subgroup of CG(E)C_{G}(E); this is reductive, and the inclusion CH(E)CG(E)C_{H}(E)\to C_{G}(E) sends a maximal torus of CH(E)C_{H}(E) into one of CG(E)C_{G}(E)^{\circ}, matching up the corresponding root data, giving (b). For (c), note that each coset of NG(E)N_{G}(E)^{\circ} in NG(E)N_{G}(E) contains a translate of NG(E)HN_{G}(E)^{\circ}\cap H, which is a maximal compact subgroup of NG(E)=CG(E)N_{G}(E)^{\circ}=C_{G}(E)^{\circ}. The union of these translates is a finite extension of a compact group, hence is compact, and therefore NH(E)N_{H}(E) meets each such coset. Identical reasoning applies for the centraliser of EE. (A more detailed justification for parts (b) and (c) can be obtained using the complexification functor from compact Lie groups to complex reductive groups, as detailed, e.g., in [26, Theorems 1 and 2].) ∎

Thus the classification of elementary abelian subgroups and their local structure in a complex reductive group can be viewed inside compact real Lie groups. We will refer in particular to [11, 22, 41].

Proposition 3.1 can already be applied to finite subgroups of NG(E)N_{G}(E) and CG(E)C_{G}(E) for an elementary abelian subgroup EGE\leq G, but stronger results are available since NG(E)N_{G}(E) and CG(E)C_{G}(E) can themselves be viewed as the points of a group scheme. The following lemma summarises a series of results of Friedlander & Mislin [20] which make use of this viewpoint. We note that the results quoted from [20] require an elementary abelian pp-subgroup with pp\neq\ell, but their proofs should also hold more generally.

Lemma 3.3.

Let K0K_{0} and KK_{\ell} be algebraically closed fields of characteristic 0 and \ell, respectively, and let pp\neq\ell be a prime. Let EE and EE^{\prime} respectively be elementary abelian pp-subgroups of G(K0)G(K_{0}) and G(K)G(K_{\ell}) which correspond under the bijection of Proposition 3.1. Then reduction-mod-\ell allows us to identify the root data of the reductive groups CG(K0)(E)C_{G(K_{0})}(E)^{\circ} and CG(K)(E)C_{G(K_{\ell})}(E^{\prime})^{\circ}, and also induces isomorphisms

NG(K0)(E)/CG(K0)(E)\displaystyle N_{G(K_{0})}(E)/C_{G(K_{0})}(E)\phantom{{{}^{\circ}}} NG(K)(E)/CG(K)(E),\displaystyle\cong N_{G(K_{\ell})}(E^{\prime})/C_{G(K_{\ell})}(E^{\prime})\phantom{{}^{\circ}},
NG(K0)(E)/CG(K0)(E)\displaystyle N_{G(K_{0})}(E)/C_{G(K_{0})}(E)^{\circ} NG(K)(E)/CG(K)(E),\displaystyle\cong N_{G(K_{\ell})}(E^{\prime})/C_{G(K_{\ell})}(E^{\prime})^{\circ},
CG(K0)(E)/CG(K0)(E)\displaystyle C_{G(K_{0})}(E)/C_{G(K_{0})}(E)^{\circ} CG(K)(E)/CG(K)(E).\displaystyle\cong C_{G(K_{\ell})}(E^{\prime})/C_{G(K_{\ell})}(E^{\prime})^{\circ}.

Moreover, the order of the component group CG(K0)(E)/CG(K0)(E)C_{G(K_{0})}(E)/C_{G(K_{0})}(E)^{\circ} is a power of pp.

Proof.

We first claim that without loss of generality we can take K0=K_{0}=\mathbb{C} and K=𝔽¯K_{\ell}=\overline{\mathbb{F}}_{\ell}, the algebraic closure of the field 𝔽\mathbb{F}_{\ell} of \ell elements. Since p\ell\neq p, all representations of a finite elementary abelian pp-group in characteristic 0 and characteristic \ell are semisimple, see Maschke’s Theorem. This shows that EE and EE^{\prime} are linearly reductive in the sense of [12, §2], thus EE and EE^{\prime} are GG-completely reducible [12, Lemma 2.6], and our first claim is then [12, Corollary 5.5].

Now we interpret EE as the \mathbb{C}-points of a finite subgroup scheme of GG, defined over an appropriate ring of Witt vectors RR, where RR comes equipped with a fixed embedding into \mathbb{C} and a surjection onto 𝔽¯\overline{\mathbb{F}}_{\ell}. By hypothesis, the image of EE in G(𝔽¯)G(\overline{\mathbb{F}}_{\ell}) is conjugate to EE^{\prime}, so we may replace EE^{\prime} by this image without loss of generality. Then NG()(E)N_{G(\mathbb{C})}(E) and NG(𝔽¯)(E)N_{G(\overline{\mathbb{F}}_{\ell})}(E^{\prime}) are the \mathbb{C}-points and 𝔽¯\overline{\mathbb{F}}_{\ell}-points of the scheme-theoretic normaliser of EE in GG, which we denote NG(E)N_{G}(E), and similarly CG()(E)C_{G(\mathbb{C})}(E) and CG(𝔽¯)(E)C_{G(\overline{\mathbb{F}}_{\ell})}(E^{\prime}) are the points of the scheme-theoretic centraliser CG(E)C_{G}(E). Then [20, Corollary 4.3 and Theorem 4.4] tell us that NG(E)N_{G}(E) and CG(E)C_{G}(E) are generalised reductive groups over RR (see [20, Definition 2.1]), and applying [20, Proposition 3.1(i)] to each of these, we deduce that the quotient by the connected component is the same over \mathbb{C} and 𝔽¯\overline{\mathbb{F}}_{\ell}. This gives the second and third isomorphisms above. The first isomorphism is derived in the proof of [20, Theorem 4.4].

Lastly, since the scheme-theoretic centraliser CG(E)C_{G}(E) is a generalised reductive group, by definition the quotient of CG(E)C_{G}(E) by its identity component is a finite étale group scheme which, by [20, Corollary 4.3], has order coprime to \ell; note that in [20] the quotient by the identity component is denoted π0()\pi_{0}(-). We can repeat this argument for any p\ell\neq p, replacing \ell and RR as appropriate, and so the order is coprime to every prime except possibly pp; in other words, its order is a pp-power. ∎

3.2. Torality

As hinted at in the introduction, the behaviour of elementary abelian subgroups admits a stark dichotomy depending on whether the subgroups in question are toral or not. In general, toral subgroups are much more well-behaved, and non-toral subgroups are comparatively rare, as illustrated by the following result of Steinberg. To state it, recall that a prime pp is called a torsion prime for a reductive group GG if some subsystem subgroup of GG has pp-torsion in its fundamental group, see [39, Definition 2.1]. Explicitly, if GG is simple then torsion primes are: pn+1p\mid n+1 for GG of type AnA_{n}; p=2p=2 for GG of type BnB_{n}, CnC_{n}, DnD_{n}, G2G_{2}; p3p\leq 3 for GG of type F4F_{4}, E6E_{6}, E7E_{7}; p5p\leq 5 for GG of type E8E_{8}; the exact possibilities depend on the isogeny type of the group and are listed in [39, Lemma 2.5] and [32, Table 9.2]. If GG is not simple, then pp is torsion for GG precisely when it is torsion for some simple factor.

Theorem 3.4 ([39, Theorem 2.28]).

Let GG be a reductive algebraic group in characteristic \ell and let pp\neq\ell be a prime. The following conditions are equivalent:

  • (a)

    The prime pp is not a torsion prime for GG.

  • (b)

    The centraliser CG(E)C_{G}(E) is connected for every elementary abelian pp-subgroup EE.

  • (c)

    Every elementary abelian pp-subgroup of GG is toral.

We close this subsection with the following useful lemma.

Lemma 3.5.

Let GG be a reductive algebraic group in characteristic \ell and let EGE\leq G be an elementary abelian pp-subgroup, where pp\neq\ell.

  • (a)

    The subgroup EE is toral in GG if and only if ECG(E)E\leq C_{G}(E)^{\circ}.

  • (b)

    Let ZGZ\leq G be central. Then EE is toral in GG if and only if EZ/ZEZ/Z is toral in G/ZG/Z.

  • (c)

    Suppose that =0\ell=0 and view the Lie algebra of GG as a KEKE-module LL with character χL\chi_{L}. Then

    dimCG(E)=1|E|xEχL(x).\dim C_{G}(E)=\frac{1}{|E|}\sum\nolimits_{x\in E}\chi_{L}(x).
Proof.

Suppose EE is contained in some maximal torus TT of GG. Since TT is connected and abelian, we have TCG(E)T\leq C_{G}(E)^{\circ} and so ECG(E)E\leq C_{G}(E)^{\circ}. Conversely, suppose ECG(E)E\leq C_{G}(E)^{\circ} and recall that CG(E)C_{G}(E)^{\circ} is reductive, see [32, Theorem 14.2]. Since the centre of a connected reductive group is contained in every maximal torus, EE is contained in every maximal torus of CG(E)C_{G}(E)^{\circ}, in particular EE is contained in some torus of GG. This proves (a). Parts (b) and (c) are proved in [11, Theorem 8.2]. ∎

3.3. Semisimple elements of small order

In our discussion of non-toral elementary abelian subgroups we will require the information provided in Table 1 below, on certain conjugacy classes of semisimple elements in exceptional groups GG. We give the centraliser of each such element gg, as well as the trace (Brauer character) χL(g)\chi_{L}(g) on the Lie algebra L(G)L(G) of GG; for GE8()G\neq E_{8}(\mathbb{C}) we also give the trace χmin(g)\chi_{\rm min}(g) on a non-trivial module of least dimension. By the results of Section 3.1, this information remains the same for the corresponding algebraic group in any characteristic coprime to the element order. These results can be obtained using the algorithm of Moody and Patera [34], but they have already appeared throughout the literature, in particular [18, Table 2], [15, Tables 4, 6], [34, Table 10], and [21, Tables 4.3.1, 4.3.2, and 4.7.1]. We have chosen our class labels to be consistent with these references.

If rr is a prime, then rkXr^{k}\text{X} stands for a conjugacy class of elements of order rkr^{k}, labelled by X. In class labels, numbers in brackets indicate that these powers form distinct conjugacy classes – for instance squares of elements in the class 3B[2]3{\rm B}[2] form a distinct class (not otherwise listed), whose traces will be the complex conjugates of the traces shown. The notation 4A[A]4{\rm A}[{\rm A}] and 4H[A]4{\rm H}[{\rm A}] indicates that the squares of these elements lie in class 2A2{\rm A}.

In the description of the centraliser, Tj(×)jT_{j}\cong(\mathbb{C}^{\times})^{j} indicates a jj-dimensional torus. The element ω3\omega_{3} is a fixed cube root of unity. The isogeny types of the groups in the centralisers can be determined from the action of the groups on L(G)L(G) and the minimal module, listed for instance in [29, §8]: the correct group is the smallest group (in the sense of taking quotients) which acts faithfully on some composition factor of L(G)L(G) if GG is adjoint, or of the minimal module if GG is simply connected of type E6E_{6} or E7E_{7}.

Table 1. Certain elements of small order in simply connected algebraic groups
𝑮\boldsymbol{G} Class 𝑪𝑮(𝒙)\boldsymbol{C_{G}(x)} 𝝌𝑳\boldsymbol{\chi_{L}} 𝝌𝐦𝐢𝐧\boldsymbol{\chi_{\rm min}}
G2()G_{2}(\mathbb{C}) 2A SL2()SL2()\operatorname{SL}_{2}(\mathbb{C})\circ\operatorname{SL}_{2}(\mathbb{C}) 2-2 1-1
F4()F_{4}(\mathbb{C}) 2A Sp6()SL2()\operatorname{Sp}_{6}(\mathbb{C})\circ\operatorname{SL}_{2}(\mathbb{C}) 4-4 22
2B Spin9()\operatorname{Spin}_{9}(\mathbb{C}) 2020 6-6
3A Sp6()T1\operatorname{Sp}_{6}(\mathbb{C})\circ T_{1} 77 88
3C SL3()SL3()\operatorname{SL}_{3}(\mathbb{C})\circ\operatorname{SL}_{3}(\mathbb{C}) 2-2 1-1
3D Spin7()T1\operatorname{Spin}_{7}(\mathbb{C})\circ T_{1} 77 1-1
E6,sc()E_{6,{\text{\rm sc}}}(\mathbb{C}) 2A SL2()SL6()\operatorname{SL}_{2}(\mathbb{C})\circ\operatorname{SL}_{6}(\mathbb{C}) 2-2 33
2B Spin10()T1\operatorname{Spin}_{10}(\mathbb{C})\circ T_{1} 1414 5-5
3A SL6()T1\operatorname{SL}_{6}(\mathbb{C})\circ T_{1} 1515 99
3B[2] SL6()T1\operatorname{SL}_{6}(\mathbb{C})\circ T_{1} 1515 9ω39\omega_{3}
3C SL3()SL3()SL3()\operatorname{SL}_{3}(\mathbb{C})\circ\operatorname{SL}_{3}(\mathbb{C})\circ\operatorname{SL}_{3}(\mathbb{C}) 3-3 0
3D Spin8()T2\operatorname{Spin}_{8}(\mathbb{C})\circ T_{2} 66 0
3E[2] E6,sc()E_{6,{\text{\rm sc}}}(\mathbb{C}) 7878 27ω327\omega_{3}
E7,sc()E_{7,{\text{\rm sc}}}(\mathbb{C}) 2A E7,sc()E_{7,{\text{\rm sc}}}(\mathbb{C}) 133133 56-56
2B SL2()Spin12()\operatorname{SL}_{2}(\mathbb{C})\circ\operatorname{Spin}_{12}(\mathbb{C}) 55 88
2C SL2()Spin12()\operatorname{SL}_{2}(\mathbb{C})\circ\operatorname{Spin}_{12}(\mathbb{C}) 55 8-8
3A SL7()T1\operatorname{SL}_{7}(\mathbb{C})\circ T_{1} 77 7-7
3B E6,sc()T1E_{6,{\text{\rm sc}}}(\mathbb{C})\circ T_{1} 5252 25-25
3C SL6()SL3()\operatorname{SL}_{6}(\mathbb{C})\circ\operatorname{SL}_{3}(\mathbb{C}) 2-2 22
3D SL2()Spin10()T1\operatorname{SL}_{2}(\mathbb{C})\circ\operatorname{Spin}_{10}(\mathbb{C})\circ T_{1} 77 22
3E Spin12()T1\operatorname{Spin}_{12}(\mathbb{C})\circ T_{1} 3434 2020
4A[A] SL8()/I\operatorname{SL}_{8}(\mathbb{C})/\left<-I\right> 7-7 0
4H[A] E6,sc()T1E_{6,{\text{\rm sc}}}(\mathbb{C})\circ T_{1} 2525 0
E8()E_{8}(\mathbb{C}) 2A SL2()E7,sc()\operatorname{SL}_{2}(\mathbb{C})\circ E_{7,{\text{\rm sc}}}(\mathbb{C}) 2424 -
2B HSpin16()\operatorname{HSpin}_{16}(\mathbb{C}) 8-8 -
3A SL9()/ω3I\operatorname{SL}_{9}(\mathbb{C})/\left<\omega_{3}I\right> 4-4 -
3B SL3()E6,sc()\operatorname{SL}_{3}(\mathbb{C})\circ E_{6,{\text{\rm sc}}}(\mathbb{C}) 55 -
3C Spin14()T1\operatorname{Spin}_{14}(\mathbb{C})\circ T_{1} 1414 -
3D E7,sc()T1E_{7,{\text{\rm sc}}}(\mathbb{C})\circ T_{1} 7777 -
5C SL5()SL5()\operatorname{SL}_{5}(\mathbb{C})\circ\operatorname{SL}_{5}(\mathbb{C}) 2-2 -

We will also refer to the inclusions of classes in Table 2, induced by the inclusions of simply connected groups F4()<E6,sc()<E7,sc()<E8()F_{4}(\mathbb{C})<E_{6,{\text{\rm sc}}}(\mathbb{C})<E_{7,{\text{\rm sc}}}(\mathbb{C})<E_{8}(\mathbb{C}). Some of this information is given in the above references, but it can also be determined directly from the character values and the known action of each group on the Lie algebra and minimal module of the next.

Table 2. Inclusions of certain conjugacy classes
F4F_{4} class E6E_{6} class E7E_{7} class E8E_{8} class
2A \to 2A \to 2B \to 2A
2B \to 2B \to 2C \to 2B
2A \to 2A

4. From algebraic groups to finite groups

Let GG be a connected reductive algebraic group over the algebraically closed field KK of characteristic >0\ell>0, with maximal torus TT and Weyl group WW. In the following we suppose that a Steinberg endomorphism FF of GG is given, that TT is FF-stable, and that we know, up to GG-conjugacy, the elementary abelian subgroups of GG with some representative in GFG^{F}, as well as their local structure in GG. Given this information, we show how to derive a classification of the elementary abelian subgroups of the finite group GFG^{F}, together with their local structure. The main tool for establishing this result is an application of the Lang-Steinberg Theorem. Note that the results of this section hold for all finite subgroups; we will return to the particular case of elementary abelian pp-subgroups in subsequent sections when applying these.

4.1. The correspondence

If AGFA\leq G^{F}, then the FF-class of a coset uNG(A)uN_{G}(A)^{\circ} in NG(A)/NG(A)N_{G}(A)/N_{G}(A)^{\circ} is the subset {F(g)ug1NG(A):gNG(A)}\{F(g)ug^{-1}N_{G}(A)^{\circ}:g\in N_{G}(A)\}. Moreover, recall that NG(A)=CG(A)N_{G}(A)^{\circ}=C_{G}(A)^{\circ} if AGA\leq G is finite.

Proposition 4.1.

Let AGA\leq G be a finite subgroup such that F(A)F(A) and AA are conjugate in GG. The following hold:

  • (a)

    There exists a GG-conjugate of AA which is FF-stable.

  • (b)

    Suppose AA has a GG-conjugate in GFG^{F}. Replacing AA by this conjugate, there is a bijection between GFG^{F}-classes of subgroups of GFG^{F} which are GG-conjugate to AA, and FF-classes in NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ} contained in CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ}: the FF-class of wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ} corresponds to the GFG^{F}-class of subgroups with representative Aw=AgA_{w}={{}^{g}}A, where gGg\in G is chosen with g1F(g)CG(A)=wg^{-1}F(g)C_{G}(A)^{\circ}=w.

Proof.

To begin, GG clearly acts on M={Ag:gG}M=\{{}^{g}A:g\in G\} transitively. Also FF acts on MM since F(A)F(A) is GG-conjugate to AA, and this action is compatible with the GG-action since F(Ag)=FF(g)(A)F({}^{g}A)={}^{F(g)}F(A) for gGg\in G. Note that AA is closed since it is finite, hence so are NG(A)N_{G}(A) and CG(A)C_{G}(A). The Lang-Steinberg Theorem then implies the existence of an FF-stable conjugate of AA, see [32, Theorem 21.11], so (a) holds, and replacing AA by such FF-stable conjugate there is a bijection between

{GF-orbits on MF}and{F-classes in NG(A)/NG(A)}.\{G^{F}\text{-orbits on }M^{F}\}\quad\text{and}\quad\{F\text{-classes in }N_{G}(A)/N_{G}(A)^{\circ}\}.

Now suppose AA is fixed point-wise by FF, so AGFA\leq G^{F}, and abbreviate W(A)=NG(A)/CG(A)W(A)=N_{G}(A)/C_{G}(A)^{\circ}. As shown in the proof of [32, Theorem 21.11], the FF-class of wW(A)w\in W(A) corresponds to the GFG^{F}-class of subgroups with representative Aw=AgA_{w}={{}^{g}}A, where gGg\in G satisfies g1F(g)CG(A)=wg^{-1}F(g)C_{G}(A)^{\circ}=w. For such an element gg, and for any aAa\in A, we have F(gag1)=F(g)aF(g)1=g(w˙aw˙1)g1F(gag^{-1})=F(g)aF(g)^{-1}=g(\dot{w}a\dot{w}^{-1})g^{-1}, for some lift w˙\dot{w} of ww to NG(A)N_{G}(A). Therefore FF acts on AwA_{w} as the map aw˙aw˙1a\mapsto\dot{w}a\dot{w}^{-1} acts on AA. In particular, AwF=AwA_{w}^{F}=A_{w} if and only if wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ}, so that the FF-class of ww consists of elements in CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ}; thus (b) holds. ∎

We note that Proposition 4.1 works for both toral and non-toral elementary abelian subgroups, and for both twisted and untwisted Steinberg morphisms. Importantly, Proposition 4.1 allows us to determine all GFG^{F}-classes of elementary abelian subgroups if we know the GG-classes of these subgroups in GG with representatives in GFG^{F} (whenever they exist). One remaining problem is to find the latter, and Corollary 4.2 below will be useful for that. Clearly, if AGA\leq G and there is gGg\in G such that B=AgGFB={}^{g}A\leq G^{F}, then F(B)=BF(B)=B and so AA and F(A)F(A) are conjugate. However, the converse is not always true. For instance, let G=GLn(K)G=\operatorname{GL}_{n}(K) where KK has characteristic 22, let TT be the subgroup of diagonal matrices, and let FF be a Steinberg morphism inducing xx2x\mapsto x^{2} on TT. Then TF=1T^{F}=1 and GFG^{F} has no elementary abelian pp-subgroups of rank nn for p2p\neq 2, even though TT contains an FF-stable elementary abelian pp-subgroup of rank nn; the action of FF on T(p)=Ω1(Op(T))T_{(p)}=\Omega_{1}(O_{p}(T)) is then non-trivial. Despite this subtlety, it remains true that for any given finite subgroup of GG, there is some FF such that GFG^{F} contains a conjugate of this subgroup, in which case the results of this section tell us exactly how many such classes arise, as well as their normaliser structure.

Corollary 4.2.

Let AGA\leq G be a finite subgroup.

  • (a)

    There is a GG-conjugate of AA in GFG^{F} if and only if AA and F(A)F(A) are GG-conjugate and there is an FF-stable GG-conjugate BB of AA such that the restriction F:BBF\colon B\to B is induced by some wNG(B)/CG(B)w\in N_{G}(B)/C_{G}(B)^{\circ}.

  • (b)

    If |NG(A)/CG(A)|=|Aut(A)||N_{G}(A)/C_{G}(A)|=|\operatorname{Aut}(A)|, then there is a GG-conjugate of AA in GFG^{F} if and only if AA and F(A)F(A) are GG-conjugate.

Proof.
  • (a)

    Suppose B=AgGFB={}^{g}A\leq G^{F} for some gGg\in G. Then BB is FF-stable and F(A)=AF(g1)gF(A)={}^{F(g^{-1})g}A is GG-conjugate to AA. The proof of Proposition 4.1 shows that FF acts on FF-stable GG-conjugates of BB as elements of NG(B)/CG(B)N_{G}(B)/C_{G}(B)^{\circ} act on BB. Conversely, suppose AA and F(A)F(A) are GG-conjugate (so FF-stable GG-conjugates exist by Proposition 4.1(a)) and that there is such a GG-conjugate B=AhB={}^{h}A such that F:BBF\colon B\to B is induced by wNG(B)/CG(B)w\in N_{G}(B)/C_{G}(B)^{\circ}, that is, F(b)=w˙bw˙1F(b)=\dot{w}b\dot{w}^{-1} for some lift w˙NG(B)\dot{w}\in N_{G}(B) of ww. If gGg\in G satisfies g1F(g)CG(B)=w1g^{-1}F(g)C_{G}(B)^{\circ}=w^{-1}, then Bg=Bw1{}^{g}B=B_{w^{-1}} is fixed point-wise by FF: if gbg1Bggbg^{-1}\in{}^{g}B with bBb\in B, then F(gbg1)=F(g)F(b)F(g)1=gw˙1F(b)w˙g1=gbg1F(gbg^{-1})=F(g)F(b)F(g)^{-1}=g\dot{w}^{-1}F(b)\dot{w}g^{-1}=gbg^{-1}, so AghGF{}^{gh}A\leq G^{F}, as claimed.

  • (b)

    This follows readily from the previous proof: using the notation of (a), the assumption on |Aut(A)||\operatorname{Aut}(A)| implies that NG(B)/CG(B)Aut(B)N_{G}(B)/C_{G}(B)\cong\operatorname{Aut}(B) for every FF-stable conjugate of AA. ∎

4.2. Local structure

We continue with the previous notation; moreover, we denote by wFwF the map given by xwF(x)w1x\mapsto wF(x)w^{-1}. The following propositions allow us to determine the local structure of the GG-conjugates of AGFA\leq G^{F} in GFG^{F} from the structure of CA(G)C_{A}(G) and NG(A)N_{G}(A).

Proposition 4.3.

Let AGFA\leq G^{F} be a finite subgroup. For wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ} let AwGFA_{w}\leq G^{F} be the GG-conjugate of AA as defined in Proposition 4.1. If w˙CG(A)\dot{w}\in C_{G}(A) is any lift of ww, then

(CG(Aw))F(CG(A))w˙F;(C_{G}(A_{w})^{\circ})^{F}\cong(C_{G}(A)^{\circ})^{\dot{w}F};

where, as usual, (CG(A))w˙F(C_{G}(A)^{\circ})^{\dot{w}F} are the fixed points of w˙F\dot{w}F in CG(A)C_{G}(A)^{\circ}. Furthermore, (CG(A))w˙F(C_{G}(A)^{\circ})^{\dot{w}F} is independent of the choice of w˙\dot{w}. If ww acts as an inner automorphism of CG(A)C_{G}(A)^{\circ}, then (CG(Aw))F(CG(A))F(C_{G}(A_{w})^{\circ})^{F}\cong(C_{G}(A)^{\circ})^{F}.

Proof.

Write C=CG(A)C=C_{G}(A). By construction, Aw=AgA_{w}={}^{g}A for some gGg\in G with g1F(g)Cg^{-1}F(g)\in C and w=g1F(g)Cw=g^{-1}F(g)C^{\circ}. Clearly, CG(Aw)=(C)gC_{G}(A_{w})^{\circ}={}^{g}(C^{\circ}). If cCc\in C^{\circ}, then F(gcg1)=F(g)F(c)F(g1)=gcg1F(gcg^{-1})=F(g)F(c)F(g^{-1})=gcg^{-1} if and only if w˙F(c)w˙1=c\dot{w}F(c)\dot{w}^{-1}=c for w˙=g1F(g)C\dot{w}=g^{-1}F(g)\in C, hence

(CG(Aw))F{cC:c=w˙F(c)w˙1}=(C)w˙F.(C_{G}(A_{w})^{\circ})^{F}\cong\{c\in C^{\circ}:c=\dot{w}F(c)\dot{w}^{-1}\}=(C^{\circ})^{\dot{w}F}.

Since AA is closed and FF-stable, so is CC. Now [21, Theorem 2.1.2(d)] proves that the restriction of FF to CC is a Steinberg endomorphism (in the sense of [21]), that is, F|CF|_{C} is surjective (hence a bijection since FF is an abstract group automorphism, hence injective) and CFC^{F} is finite. In particular, F|CF|_{C} is a Steinberg endomorphism in the sense of [32] and as considered here. It follows from [21, Proposition 1.1.4(c)] that F(C)CF(C^{\circ})\leq C^{\circ}, so CC^{\circ} is FF-stable, and now [32, Exercise 30.1] shows that F|CF|_{C^{\circ}} is a bijection. In conclusion, FF induces a Steinberg automorphism of CC^{\circ}. If cw˙c\dot{w} with cCc\in C^{\circ} is another lift of ww, then the restrictions of w˙F\dot{w}F and cw˙Fc\dot{w}F to CC^{\circ} differ by an inner automorphism of CC^{\circ}, and [32, Corollary 21.8] shows that (C)w˙F(C^{\circ})^{\dot{w}F} and (C)cw˙F(C^{\circ})^{c\dot{w}F} are isomorphic, as claimed. In particular, if ww induces an inner automorphism on CC^{\circ}, then the map wFwF equals cFcF for some cCc\in C^{\circ}, and (C)wF=(C)cF(C)F(C^{\circ})^{wF}=(C^{\circ})^{cF}\cong(C^{\circ})^{F}. ∎

Proposition 4.4.

Let AGFA\leq G^{F} be a finite subgroup, let wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ}, and let AwGFA_{w}\leq G^{F} be the GG-conjugate of AA under the correspondence in Proposition 4.1. Then

NG(Aw)F/(CG(Aw))F\displaystyle N_{G}(A_{w})^{F}/(C_{G}(A_{w})^{\circ})^{F} (NG(A)/CG(A))wF,\displaystyle\cong(N_{G}(A)/C_{G}(A)^{\circ})^{wF},
CG(Aw)F/(CG(Aw))F\displaystyle C_{G}(A_{w})^{F}/(C_{G}(A_{w})^{\circ})^{F} (CG(A)/CG(A))wF.\displaystyle\cong(C_{G}(A)/C_{G}(A)^{\circ})^{wF}.
Proof.

Write C=CG(A)C=C_{G}(A) and N=NG(A)N=N_{G}(A). By construction, we have Aw=gAg1A_{w}=gAg^{-1} for some gGg\in G such that g1F(g)C=wg^{-1}F(g)C^{\circ}=w. Let w˙=g1F(g)C\dot{w}=g^{-1}F(g)\in C. If nNn\in N, then

gng1NG(Aw)Fgng1=F(gng1)=F(g)F(n)F(g)1=gw˙F(n)w˙1g1w˙F(n)w˙1=nNw˙F.\displaystyle\begin{array}[]{lrl}&gng^{-1}&\in N_{G}(A_{w})^{F}\\[2.15277pt] \iff&gng^{-1}&=F(gng^{-1})=F(g)F(n)F(g)^{-1}=g\dot{w}F(n)\dot{w}^{-1}g^{-1}\\[2.15277pt] \iff&\dot{w}F(n)\dot{w}^{-1}&=n\in N^{\dot{w}F}.\end{array}

Thus, we have an isomorphism NG(Aw)FNw˙FN_{G}(A_{w})^{F}\cong N^{\dot{w}F}, which also induces isomorphisms CG(Aw)FCw˙FC_{G}(A_{w})^{F}\cong C^{\dot{w}F}, (CG(Aw))F(C)w˙F(C_{G}(A_{w})^{\circ})^{F}\cong(C^{\circ})^{\dot{w}F}, and (NG(Aw))F(N)w˙F(N_{G}(A_{w})^{\circ})^{F}\cong(N^{\circ})^{\dot{w}F}. Since GG is connected, [21, Theorem 2.1.2(f)] shows that GFG^{F} and Gw˙FG^{\dot{w}F} are GG-conjugate, hence both finite. Since w˙F\dot{w}F is also bijective on GG, it is a Steinberg morphism (in the sense of [21]). Recall that NN and CC are closed and mapped under w˙F\dot{w}F into themselves. Now [21, Theorem 2.1.2(d)] shows that wFwF induces Steinberg morphisms on NN and on CC, respectively. Applying [21, Theorem 2.1.2(d)] to NN and to CC, respectively, we see that w˙F\dot{w}F maps NN^{\circ} and CC^{\circ} onto themselves and that the natural maps Nw˙F(N/N)w˙FN^{\dot{w}F}\to(N/N^{\circ})^{\dot{w}F} and Cw˙F(C/C)w˙FC^{\dot{w}F}\to(C/C^{\circ})^{\dot{w}F} are surjective. The claim follows. ∎

4.3. The FF-action on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}

The previous results require us to study the action of FF on the normaliser quotient.

Proposition 4.5.

Let AGFA\leq G^{F} be a finite subgroup. The map NG(A)NG(A)N_{G}(A)\to N_{G}(A) induced by FF is given by nnϕ(n)n\mapsto n\phi(n), where ϕ\phi is a 11-cocycle NG(A)CG(A)N_{G}(A)\to C_{G}(A), that is, ϕ\phi satisfies

ϕ(n1n2)=(ϕ(n1)n2)ϕ(n2)\phi(n_{1}n_{2})=(\phi(n_{1})^{n_{2}})\phi(n_{2})

for all n1,n2NG(A)n_{1},n_{2}\in N_{G}(A). In particular, FF induces the identity map on NG(A)/CG(A)N_{G}(A)/C_{G}(A).

Proof.

By hypothesis, if nNG(A)n\in N_{G}(A) and aAa\in A then n1an=F(n1an)=F(n)1aF(n)n^{-1}an=F(n^{-1}an)=F(n)^{-1}aF(n), thus F(n)n1CG(A)F(n)n^{-1}\in C_{G}(A) and the first statement holds. Writing F(n)=nϕ(n)F(n)=n\phi(n), we have n1n2ϕ(n1n2)=F(n1n2)=F(n1)F(n2)=n1ϕ(n1)n2ϕ(n2)n_{1}n_{2}\phi(n_{1}n_{2})=F(n_{1}n_{2})=F(n_{1})F(n_{2})=n_{1}\phi(n_{1})n_{2}\phi(n_{2}), from which the cocycle condition on ϕ\phi follows. ∎

While FF acts trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A), it does not necessarily act trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}, even if the action on CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ} is trivial:

Example 4.6.

Let G=SL2(K)G=\operatorname{SL}_{2}(K) and GF=SL2(3)G^{F}=\operatorname{SL}_{2}(3), with FF induced by xx3x\mapsto x^{3}. Let AGFA\leq G^{F} be a Sylow 22-subgroup and note that AGFA\unlhd G^{F} and CG(A)={±I2}C_{G}(A)=\{\pm I_{2}\}. If α\alpha is a primitive element of 𝔽9\mathbb{F}_{9}, then m=diag(α2,α6)NG(A)m=\operatorname{diag}(\alpha^{2},\alpha^{6})\in N_{G}(A) satisfies F(m)I2m1=I2F(m)\cdot I_{2}\cdot m^{-1}=-I_{2}. This shows that there is only one FF-class of NG(A)N_{G}(A)-orbits in CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ}. In particular, FF acts as the identity on NG(A)/CG(A)N_{G}(A)/C_{G}(A), see Proposition 4.5, and on CG(A)/CG(A)=CG(A)={±I2}C_{G}(A)/C_{G}(A)^{\circ}=C_{G}(A)=\{\pm I_{2}\}, but FF acts non-trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}.

If FF acts trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}, then Propositions 4.3 and 4.4 have the following corollary:

Corollary 4.7.

Let AGFA\leq G^{F} be finite. If FF acts trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}, then there is a bijection between the NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}-classes in CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ} and the GFG^{F}-classes of subgroups of GFG^{F} that are GG-conjugate to AA; this bijection maps an element wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ} to AwGFA_{w}\leq G^{F}, as defined in the correspondence in Proposition 4.1; moreover

CGF(Aw)=(CG(Aw))F=(CG(A))wF.CCG(A)/CG(A)(w),C_{G^{F}}(A_{w})=(C_{G}(A_{w}))^{F}=(C_{G}(A)^{\circ})^{wF}.C_{C_{G}(A)/C_{G}(A)^{\circ}}(w),

and

NGF(Aw)=(NG(Aw))F=(CG(A))wF.CNG(A)/CG(A)(w).N_{G^{F}}(A_{w})=(N_{G}(A_{w}))^{F}=(C_{G}(A)^{\circ})^{wF}.C_{N_{G}(A)/C_{G}(A)^{\circ}}(w).

4.4. Cohomology

Recall from [36, I.§5] that if NN is a group which acts on a group CC by automorphisms, then the cohomology set H1(N,C)H^{1}(N,C) is the set of all 11-cocycles, modulo the equivalence relation \sim where ϕψ\phi\sim\psi if there exists cCc\in C such that ϕ(n)=(cn)ψ(n)(c1)\phi(n)=(c^{n})\psi(n)(c^{-1}) for all nNn\in N. When CC is abelian, this coincides with the usual definition of H1H^{1} via right-derived functors of Hom. In general, H1(N,C)H^{1}(N,C) is not a group, but a pointed set, the distinguished point 0 given by the class of the map n1n\mapsto 1 for all nNn\in N.

The next result shows that for certain AGFA\leq G^{F} and given NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ} in the algebraic group, we find a GG-conjugate BGFB\leq G^{F} with the same normaliser quotient in GFG^{F}.

Corollary 4.8.

Let AGFA\leq G^{F} be a finite subgroup with H1(NG(A),CG(A))={0}H^{1}(N_{G}(A),C_{G}(A))=\{0\}. There exists a subgroup BGFB\leq G^{F} which is GG-conjugate to AA, such that

NG(B)F/(CG(B))F\displaystyle N_{G}(B)^{F}/(C_{G}(B)^{\circ})^{F} NG(A)/CG(A),and\displaystyle\cong N_{G}(A)/C_{G}(A)^{\circ},\ \text{and}
CG(B)F/(CG(B))F\displaystyle C_{G}(B)^{F}/(C_{G}(B)^{\circ})^{F} CG(A)/CG(A).\displaystyle\cong C_{G}(A)/C_{G}(A)^{\circ}.

Moreover, the FF-classes of NG(B)/CG(B)N_{G}(B)/C_{G}(B)^{\circ} are precisely the conjugacy classes of NG(B)/CG(B)N_{G}(B)/C_{G}(B)^{\circ}, and for the FF-stable conjugate BwB_{w} corresponding to the FF-class of wCG(B)/CG(B)w\in C_{G}(B)/C_{G}(B)^{\circ} we have

NG(Bw)F/(CG(Bw))F\displaystyle N_{G}(B_{w})^{F}/(C_{G}(B_{w})^{\circ})^{F} CNG(B)/CG(B)(w),and\displaystyle\cong C_{N_{G}(B)/C_{G}(B)^{\circ}}(w),\ \text{and}
CG(Bw)F/(CG(Bw))F\displaystyle C_{G}(B_{w})^{F}/(C_{G}(B_{w})^{\circ})^{F} CCG(B)/CG(B)(w).\displaystyle\cong C_{C_{G}(B)/C_{G}(B)^{\circ}}(w).
Proof.

The hypothesis implies that every 11-cocycle is of the form n(cn)c1n\mapsto(c^{n})c^{-1} for some cCG(A)c\in C_{G}(A). Thus, by Proposition 4.5, there is cCG(A)c\in C_{G}(A) such that F:NG(A)NG(A)F\colon N_{G}(A)\to N_{G}(A), ncnc1n\mapsto cnc^{-1}. Now define B=AuB=A_{u} as the FF-stable GG-conjugate of AA corresponding to the FF-class of u=c1CG(A)u=c^{-1}C_{G}(A)^{\circ}, so that the first claim follows from Proposition 4.4. Recall that we can define B=gAg1B=gAg^{-1} for some gGg\in G with F(g)CG(A)=gc1CG(A)F(g)C_{G}(A)^{\circ}=gc^{-1}C_{G}(A)^{\circ}. Since F(n)=cnc1F(n)=cnc^{-1} for all nNG(A)n\in N_{G}(A) and F(g)=gc1c~F(g)=gc^{-1}\tilde{c} for some c~CG(A)\tilde{c}\in C_{G}(A)^{\circ}, it follows that every mCG(B)NG(B)/CG(B)mC_{G}(B)^{\circ}\in N_{G}(B)/C_{G}(B)^{\circ} is fixed by FF. Together with Proposition 4.4, this implies the second claim. ∎

5. Toral subgroups of simple algebraic groups

Recall the notation we have fixed in Section 2, with GG a simple algebraic group in characteristic \ell. Using [22, (2.13)(iii)], we can assume that a given elementary abelian pp-subgroup EE (with p)p\neq\ell) is contained in the normaliser NG(T)N_{G}(T) of our fixed maximal torus TT of GG. We study separately the cases that EE is toral or non-toral: in the former case we assume that ETE\leq T; in the latter case, EE has non-trivial image in the Weyl group W=NG(T)/TW=N_{G}(T)/T.

Our goal in this section is to describe a practical algorithm for enumerating such toral elementary abelian pp-groups and determining their normaliser structure. We begin with Proposition 5.1 (as stated below) which simplifies our calculations: Part (a) enables us to deduce all relevant information working solely within NG(T)N_{G}(T). Part (b) then allows us to describe the normaliser of a toral subgroup by splitting it into canonical sub-quotients which can be studied separately and recombined. Following this proposition, in Section 5.1 we then describe our algorithm for enumerating elementary abelian subgroups and determining their normaliser structure. Finally, in Section 5.2 we describe a process for extending this classification of subgroups of GG to a classification of subgroups in the corresponding finite groups of Lie type, that is, in GFG^{F}.

Much of the argument below applies equally well to arbitrary abelian subgroups (not just elementary abelian), but we concentrate on elementary abelian subgroups for two reasons: Firstly, methods from linear algebra can be brought to bear, allowing for a very efficient classification algorithm (see Section 5.1 and our implementation [7]); secondly, as explained in the introduction, elementary abelian subgroups have many interesting applications, for example, in the classification of maximal pp-local and pp-radical subgroups.

In the following, recall that A.BA.B indicates a (possibly non-split) extension with normal subgroup AA and quotient BB.

Proposition 5.1.

Let GG be a simple algebraic group, with maximal torus TT and Weyl group WW. If A,BTA,B\leq T are finite subgroups, then the following hold.

  • (a)

    If A=BgA=B^{g} with gGg\in G, then g=vcg=vc for some vNG(T)v\in N_{G}(T) and cCG(A)c\in C_{G}(A)^{\circ}; in particular, AA and BB are conjugate in NG(T)N_{G}(T).

  • (b)

    We can decompose NG(A)(CG(A).(CG(A)/CG(A))).(NG(A)/CG(A))N_{G}(A)\cong(C_{G}(A)^{\circ}.(C_{G}(A)/C_{G}(A)^{\circ})).(N_{G}(A)/C_{G}(A)), with isomorphisms

    CG(A)/CG(A)\displaystyle C_{G}(A)/C_{G}(A)^{\circ} \displaystyle\cong CW(A)/W(CG(A))and\displaystyle C_{W}(A)/W(C_{G}(A)^{\circ})\quad\text{and}
    NG(A)/CG(A)\displaystyle N_{G}(A)/C_{G}(A) \displaystyle\cong NW(A)/CW(A),\displaystyle N_{W}(A)/C_{W}(A),

    where W(CG(A))W(C_{G}(A)^{\circ}) is the Weyl group of the reductive group CG(A)C_{G}(A)^{\circ}.

Proof.
  • (a)

    Note that ATTgA\leq T\cap T^{g}. If aAa\in A, then aa is semisimple, and [32, Theorem 14.2] shows that CG(a)C_{{G}}(a)^{\circ} is a connected reductive group containing T{T} and TgT^{g}. Since AA is finite, induction proves that CG(A)C_{{G}}(A)^{\circ} contains TT and TgT^{g}; these are therefore CG(A)C_{G}(A)^{\circ}-conjugate, hence T=Tgc{T}={T}^{gc} for some cCG(A)c\in C_{G}(A)^{\circ}, that is, gcNG(T)gc\in N_{G}({T}).

  • (b)

    In the following, write C=CG(A)C=C_{G}(A); clearly, NG(A)=C.(C/C).(NG(A)/C)N_{G}(A)=C^{\circ}.(C/C^{\circ}).(N_{G}(A)/C). It follows from Part (a) that NG(A)=NNG(T)(A)C=NNG(T)(A)CN_{G}(A)=N_{N_{G}(T)}(A)C^{\circ}=N_{N_{G}(T)}(A)C, and so

    NG(A)/C\displaystyle N_{G}(A)/C \displaystyle\cong NNG(T)(A)/(NNG(T)(A)C)\displaystyle N_{N_{G}(T)}(A)/(N_{N_{G}(T)}(A)\cap C)
    \displaystyle\cong (NNG(T)(A)/T)/(CNG(T)(A)/T)\displaystyle(N_{N_{G}(T)}(A)/T)/(C_{N_{G}(T)}(A)/T)
    =\displaystyle= NW(A)/CW(A).\displaystyle N_{W}(A)/C_{W}(A).

    Note that

    NNG(T)(A)C/C\displaystyle N_{N_{G}(T)}(A)C^{\circ}/C^{\circ} \displaystyle\cong NNG(T)(A)/(NNG(T)(A)C)\displaystyle N_{N_{G}(T)}(A)/(N_{N_{G}(T)}(A)\cap C^{\circ})
    \displaystyle\cong NW(A)/(NC(T)/T)\displaystyle N_{W}(A)/(N_{C^{\circ}}(T)/T)
    =\displaystyle= NW(A)/W(C).\displaystyle N_{W}(A)/W(C^{\circ}).

    These isomorphisms allow us to identify C/CNNG(T)(A)C/CC/C^{\circ}\leq N_{N_{G}(T)}(A)C^{\circ}/C^{\circ} as a subgroup of NW(A)/W(C)N_{W}(A)/W(C^{\circ}), and we deduce C/CCNW(A)/W(C)(A)=CW(A)/W(C)C/C^{\circ}\cong C_{N_{W}(A)/W(C^{\circ})}(A)=C_{W}(A)/W(C^{\circ}). ∎

5.1. Computation of toral elementary abelian subgroups

Continuing with the previous notation, we now explain how to classify, up to conjugacy, the toral elementary abelian pp-subgroups of GG algorithmically, by working in a suitably-chosen finite group of Lie type. For technical reasons, we first assume that pp is odd, and treat the case p=2p=2 in a moment.

Recall that TT is a fixed maximal torus of GG with corresponding set of roots Φ\Phi. First, by Dirichlet’s Theorem we can choose a prime-power qq such that pp divides q1q-1; by Proposition 3.1, we may assume that the characteristic \ell divides qq. Second, we can choose a Steinberg morphism FF of GG which induces the qq-power map on TT. This gives rise to the finite group GFG^{F}, containing the fixed-point subgroup TFT^{F} which is a product of cyclic groups of order q1q-1. The subgroup T(p)T_{(p)} of TFT^{F} is defined as T(p)=Ω1(Op(T))T_{(p)}=\Omega_{1}(O_{p}(T)); it contains a representative of each toral elementary abelian pp-subgroup of GG.

Recall from Proposition 5.1(a) that two toral subgroups of TT are conjugate in GG if and only if they are conjugate under the action of the Weyl group W=NG(T)/TW=N_{G}(T)/T. In GFG^{F} we therefore consider the extended Weyl group VV of GFG^{F}, see [38, Notation 2.1]. Originally defined by Tits [40, § 4.6] when GG is simply connected, VV is the subgroup of GG generated by elements nα(1)=xα(1)xα(1)xα(1)n_{\alpha}(1)=x_{\alpha}(1)x_{-\alpha}(-1)x_{\alpha}(1), where x±α(±1)x_{\pm\alpha}(\pm 1) are root elements of GG and α\alpha ranges over the simple roots of GG. By construction VNG(T)V\leq N_{G}(T), and VTV\cap T is an elementary abelian subgroup of order gcd(2,1)r\gcd(2,\ell-1)^{r}, where rr is the rank of GG; the corresponding quotient is the Weyl group WW. Specifically, VV normalises TFT^{F}, and VTF/TFWVT^{F}/T^{F}\cong W. Our choice of FF and [14, Section 12.1 and p. 61] imply that VGFV\leq G^{F}, and therefore the action of WW on T(p)T_{(p)} can be viewed inside the finite group VTFGFVT^{F}\leq G^{F}. In our setting, GG may not be simply connected but the same definition V=nα(1):α a simple rootV=\left<n_{\alpha}(1):\alpha\text{ a simple root}\right> still produces a subgroup normalising TT and TFT^{F}, and mapping surjectively to WW under the quotient map NG(T)WN_{G}(T)\to W. We compute W~GLr(p)\tilde{W}\leq\operatorname{GL}_{r}(p) as the image of VV defined by its action on T(p)T_{(p)}, and we determine all toral elementary abelian pp-subgroups of GG, up to conjugacy, by computing the W~\tilde{W}-conjugacy classes of elementary abelian subgroups contained in T(p)T_{(p)}. In the following, let EE be such an elementary abelian subgroup; we now describe how to determine the structure of NG(E)N_{G}(E) within GFG^{F}.

By Proposition 5.1(b), to describe the structure of NG(E)N_{G}(E) we need to determine CG(E)C_{G}(E)^{\circ} and the finite groups CW(E)/W(CG(E))C_{W}(E)/W(C_{G}(E)^{\circ}) and NW(E)/CW(E)N_{W}(E)/C_{W}(E). As in the proof of Proposition 5.1(a), it follows from [32, Theorem 14.2] and a finite inductive argument that CG(E)C_{G}(E)^{\circ} is generated by TT and those root subgroups Uα={xα(c):cK}U_{\alpha}=\{x_{\alpha}(c):c\in K\} which commute with EE. To find which root subgroups we need, it suffices to check which of the finitely many elements xα(1)x_{\alpha}(1) commute with EE; note that each xα(1)x_{\alpha}(1) lies in GFG^{F} by our choice of FF. This allows us to compute the root datum of CG(E)C_{G}(E)^{\circ}. Since TCG(E)T\leq C_{G}(E)^{\circ}, adding a suitable toral subgroup determines most of the structure of CG(E)C_{G}(E)^{\circ}; the remaining work is to determine the isogeny types of the occurring simple factors in CG(E)C_{G}(E)^{\circ}. It now remains to understand CW(E)/W(CG(E))C_{W}(E)/W(C_{G}(E)^{\circ}) and NW(E)/CW(E)N_{W}(E)/C_{W}(E). The action of W=NG(T)/TW=N_{G}(T)/T on TT restricts to an action on the characteristic subgroup T(p)T_{(p)}, giving a surjective homomorphism WW~W\to\tilde{W}. The only algebraic endomorphisms of the multiplicative group K×K^{\times} are power maps, and it follows that the full group of algebraic automorphisms of TT is isomorphic to GLr()\operatorname{GL}_{r}(\mathbb{Z}). Moreover, the restriction to T(p)T_{(p)} is precisely the homomorphism GLr()GLr(p)\operatorname{GL}_{r}(\mathbb{Z})\to\operatorname{GL}_{r}(p) given by reducing matrix entries modulo pp. Restricting this map to the finite subgroup WAut(T)W\leq\operatorname{Aut}(T) gives us the above map WW~W\to\tilde{W}. A result of Minkowski [33], see also [37, Lemma 1], tells us that the kernel of GLr()GLr(/m)\operatorname{GL}_{r}(\mathbb{Z})\to\operatorname{GL}_{r}(\mathbb{Z}/m\mathbb{Z}) is torsion-free for all integers m>2m>2, thus the induced map WW~W\to\tilde{W} is injective. This proves that we can compute the entire structure of NW(E)N_{W}(E) inside W~\tilde{W}; in conclusion, the structure of NG(E)N_{G}(E) is determined.

When p=2p=2, the above argument goes through similarly, with the exception that Minkowski’s Lemma fails to apply to the map GLr()GLr(/2)\operatorname{GL}_{r}(\mathbb{Z})\to\operatorname{GL}_{r}(\mathbb{Z}/2\mathbb{Z}); indeed, the kernel can contain elements of order 22 in this case. For this reason, instead of working with T(2)T_{(2)}, we pick qq so that 4q14\mid q-1, and let T(4)=Ω2(O2(T))T_{(4)}=\Omega_{2}(O_{2}(T)) be the characteristic subgroup of TT generated by elements of order dividing 44. Then the WW-orbits on elementary abelian 22-subgroups of TT coincide with the W~\tilde{W}-orbits on elementary abelian 22-subgroups of T(4)T_{(4)}, where W~\tilde{W} is the image of WW in Aut(T(4))=GLr(/4)\operatorname{Aut}(T_{(4)})=\operatorname{GL}_{r}(\mathbb{Z}/4\mathbb{Z}). We can now apply Minkowski’s Lemma as above to deduce that the map WW~W\to\tilde{W} is an isomorphism. This proves that for each elementary abelian 22-subgroup ETE\leq T, the structure of NG(E)N_{G}(E) is again determined by working in the finite group NW~(E)N_{\tilde{W}}(E).

A Magma implementation of this algorithm is available at [7].

5.2. Translation to finite groups

We use the notation of Section 4, that is, GG is a connected reductive algebraic group over the algebraically closed field KK of characteristic \ell, with maximal torus TT and Weyl group WW. The prime pp is different from \ell, and FF is a (possibly twisted) Steinberg endomorphism GG such that TT is FF-stable. The aim of this section is to describe how to classify, up to GFG^{F}-conjugacy, the toral elementary abelian subgroups of GFG^{F}, together with their local structure in GFG^{F}, assuming that this information is known for GG. The approach is based on the following lemma (and results of Section 4), and summarised in the subsequent remark.

Lemma 5.2.

If ATGFA\leq T\cap G^{F} is toral, then

NG(A)/CG(A)\displaystyle N_{G}(A)/C_{G}(A)^{\circ} =NGF(A)/(CG(A))Fand\displaystyle=N_{G^{F}}(A)/(C_{G}(A)^{\circ})^{F}\quad\text{and}
CG(A)/CG(A)\displaystyle C_{G}(A)/C_{G}(A)^{\circ} =CGF(A)/(CG(A))F,\displaystyle=C_{G^{F}}(A)/(C_{G}(A)^{\circ})^{F},

and FF acts trivially on NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}.

Proof.

Let NG(A)NG(A)/CG(A)N_{G}(A)\to N_{G}(A)/C_{G}(A)^{\circ} be the natural projection. Its restriction to NGF(A)N_{G^{F}}(A) has kernel CG(A)GF=(CG(A))FC_{G}(A)^{\circ}\cap G^{F}=(C_{G}(A)^{\circ})^{F}; thus, the first claim follows if we show that this restriction is surjective. For this recall that the extended Weyl group VGFV\leq G^{F} satisfies NG(T)=T,VN_{G}(T)=\langle T,V\rangle, see Section 5.1. Moreover, Proposition 5.1 shows that if gNG(A)g\in N_{G}(A), then g=vcg=vc for some vNG(T)v\in N_{G}(T) and cCG(A)c\in C_{G}(A)^{\circ}. Since NG(T)=V,TN_{G}(T)=\langle V,T\rangle and TCG(A)T\leq C_{G}(A)^{\circ}, we can assume that vNGF(A)v\in N_{G^{F}}(A) and cCG(A)c\in C_{G}(A)^{\circ}; this shows that NGF(A)NG(A)/CG(A)N_{G^{F}}(A)\to N_{G}(A)/C_{G}(A)^{\circ} is surjective. The claim about the centralisers follows analogously. ∎

Remark 5.3.

For a simple algebraic group GG, to classify all toral elementary abelian pp-subgroups of GFG^{F} up to conjugacy, we now have the following recipe.

  • (a)

    Determine the toral elementary abelian pp-subgroups AGA\leq G and their local structure, up to GG-conjugacy. This can be done with the method described in Section 5.1. For each GG-class, determine a GG-class representative AA that lies in GFG^{F} (if such a representative exists); Corollary 4.2 is useful here.

  • (b)

    For each such representative AGFA\leq G^{F}, determine the NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}-classes in CG(A)/CG(A)C_{G}(A)/C_{G}(A)^{\circ}.

  • (c)

    For each NG(A)/CG(A)N_{G}(A)/C_{G}(A)^{\circ}-class representative wCG(A)/CG(A)w\in C_{G}(A)/C_{G}(A)^{\circ}, determine the local structure of AwGFA_{w}\leq G^{F} using Corollary 4.7; note that this corollary is applicable due to Lemma 5.2.

In Step (b), we note that if CG(A)=CG(A)C_{G}(A)=C_{G}(A)^{\circ}, then the GG-class of AA contains only one GFG^{F}-class, and CGF(A)=CG(A)FC_{G^{F}}(A)=C_{G}(A)^{F} and NGF(A)=CG(A)F.(NG(A)/CG(A))N_{G^{F}}(A)=C_{G}(A)^{F}.(N_{G}(A)/C_{G}(A)). If CG(A)CG(A)C_{G}(A)\neq C_{G}(A)^{\circ}, then pp is a torsion prime by Theorem 3.4, and some work is required in Step (c).

6. Non-toral subgroups of exceptional algebraic groups

We now turn our attention to non-toral elementary abelian subgroups. In this case, the analogue of Proposition 5.1 fails, that is, the normaliser structure of such a subgroup is not controlled by the normaliser of a maximal torus, and thus more ad-hoc calculations are required. Nevertheless the results of Section 3.1 still apply, allowing us to transfer many known results from the characteristic 0 setting.

Let GG be an exceptional simple algebraic group, still over an algebraically closed field KK of characteristic \ell, different from a fixed prime pp. Each non-toral elementary abelian pp-subgroup of GG is contained in a maximal such subgroup, which have been classified up to conjugacy by Griess [22] for groups over \mathbb{C}. Also for complex groups, when pp is odd, a complete description of non-toral elementary abelian pp-subgroups and their normaliser structure is given by [11, Section 8]. When p=2p=2 and GG is adjoint, much information regarding the collection of all elementary abelian 22-subgroups is given in [41]. Comparing this with the information on toral subgroups provided by our algorithm, this allows us to derive a complete list of non-toral subgroups, and it then remains to determine properties of these subgroups.

We summarise these results in the subsequent tables. In these tables, we also give the distribution of elements among the conjugacy classes of the group GG. For an elementary abelian pp-subgroup EE of GG, and for conjugacy classes of order-pp elements of GG labelled pXp\text{X}, pYp\text{Y}, pZp\text{Z} etc. in Table 1, we write Dist(E)=pXaYbZc\operatorname{Dist}(E)=p\text{X}_{a}\text{Y}_{b}\text{Z}_{c}\cdots to indicate that |EpX|=a|E\cap p\text{X}|=a, |EpY|=b|E\cap p\text{Y}|=b, and so on. So for instance in Table 3, the group labelled (33)c(3^{3})_{c} has two elements in class 3C3{\rm C} and twenty-four in class 3D3{\rm D} (together accounting for all non-identity elements).

6.1. Statement of results for odd pp

In view of Proposition 3.1 and Lemma 3.3, the next proposition follows from [22, §1] and [11, §8]. The class distribution of the non-toral subgroup in F4F_{4} is derived in the proof of [22, Theorem 7.4].

Proposition 6.1 (Griess; Andersen et al.).

Let pp be an odd prime and let GG be a simple algebraic group of exceptional type over an algebraically closed field KK of characteristic p\ell\neq p. If EGE\leq G is a non-toral elementary abelian pp-subgroup, then p{3,5}p\in\{3,5\} and (G,E)(G,E) appears in Table 3. Each line of the table corresponds to a unique GG-conjugacy class; supplementing comments are given in Remark 6.2.

Table 3. Non-toral elementary abelian pp-subgroups of exceptional algebraic groups, pp odd
𝑮\boldsymbol{G} 𝑬\boldsymbol{E} 𝐃𝐢𝐬𝐭(𝑬)\boldsymbol{\operatorname{Dist}(E)} 𝑪𝑮(𝑬)\boldsymbol{C_{G}(E)} 𝑵𝑮(𝑬)\boldsymbol{N_{G}(E)}
E8E_{8} 535^{3} 5C1245{\rm C}_{124} 535^{3} 53:SL3(5)5^{3}\mathpunct{:}\operatorname{SL}_{3}(5)
F4F_{4} 333^{3} 3C263{\rm C}_{26} 333^{3} 33:SL3(3)3^{3}\mathpunct{:}\operatorname{SL}_{3}(3)
E6,scE_{6,{\text{\rm sc}}} 343^{4} 3C78E1E13{\rm C}_{78}^{\phantom{1}}{\rm E}_{1}^{\phantom{1}}{\rm E}^{\prime}_{1} 343^{4} 31+3+3:SL3(3)3^{1+3+3}\mathpunct{:}\operatorname{SL}_{3}(3)
\cdashline2-5 333^{3} 3C263{\rm C}_{26} 343^{4} 3×(33:SL3(3))3\times(3^{3}\mathpunct{:}\operatorname{SL}_{3}(3))
E6,adE_{6,{\text{\rm ad}}} (34)a(3^{4})_{a} 3C62D183{\rm C}_{62}{\rm D}_{18} (34)a(3^{4})_{a} (34).((32×32):(3×GL2(3)))(3^{4}).((3^{2}\times 3^{2})\mathpunct{:}(3\times\operatorname{GL}_{2}(3)))
(34)b(3^{4})_{b} 3AB6C50D243{\rm AB}_{6}{\rm C}_{50}{\rm D}_{24} 32×T23^{2}\times T_{2} (32×T2).(32:(Dih12×SL2(3)))(3^{2}\times T_{2}).(3^{2}\mathpunct{:}(\operatorname{Dih}_{12}\times\operatorname{SL}_{2}(3)))
\cdashline2-5 (33)a(3^{3})_{a} 3C20D63{\rm C}_{20}{\rm D}_{6} 32×(T2:3)3^{2}\times(T_{2}:3) (32×(T2:3)).(3+1+2:22)(3^{2}\times(T_{2}:3)).(3^{1+2}_{+}:2^{2})
(33)b(3^{3})_{b} 3C263{\rm C}_{26} (33)b.(33)(3^{3})_{b}.(3^{3}) (33)b.(33:SL3(3))(3^{3})_{b}.(3^{3}\mathpunct{:}\operatorname{SL}_{3}(3))
(33)c(3^{3})_{c} 3C2D243{\rm C}_{2}{\rm D}_{24} 32×SL3(K)3^{2}\times\operatorname{SL}_{3}(K) (32×SL3(K)).(32:(2×SL2(3)))(3^{2}\times\operatorname{SL}_{3}(K)).(3^{2}\mathpunct{:}(2\times\operatorname{SL}_{2}(3)))
(33)d(3^{3})_{d} 3AB2C16D83{\rm AB}_{2}{\rm C}_{16}{\rm D}_{8} 32×GL2(K)3^{2}\times\operatorname{GL}_{2}(K) (32×GL2(K)).(2×SL2(3))(3^{2}\times\operatorname{GL}_{2}(K)).(2\times\operatorname{SL}_{2}(3))
\cdashline2-5 (32)a(3^{2})_{a} 3C6D23{\rm C}_{6}{\rm D}_{2} 32×PSL3(K)3^{2}\times\operatorname{PSL}_{3}(K) (32×PSL3(K)).6(3^{2}\times\operatorname{PSL}_{3}(K)).6
(32)b(3^{2})_{b} 3D83{\rm D}_{8} 32×G2(K)3^{2}\times G_{2}(K) (32×G2(K)).SL2(3)(3^{2}\times G_{2}(K)).\operatorname{SL}_{2}(3)
E7E_{7} 343^{4} 3B2C783{\rm B}_{2}{\rm C}_{78} (33×T1)(3^{3}\times T_{1}) (33×T1).((33.SL3(3)):2)(3^{3}\times T_{1}).((3^{3}.\operatorname{SL}_{3}(3))\mathpunct{:}2)
\cdashline2-5 333^{3} 3C263{\rm C}_{26} (33×SL2(K))/Z(3^{3}\times\operatorname{SL}_{2}(K))/Z (33:SL3(3))×SL2(K)/Z(3^{3}\mathpunct{:}\operatorname{SL}_{3}(3))\times\operatorname{SL}_{2}(K)/Z
E8E_{8} (35)a(3^{5})_{a} 3A156B80D63{\rm A}_{156}{\rm B}_{80}{\rm D}_{6} 33×T23^{3}\times T_{2} (33×T2).(34:(22×SL3(3)))(3^{3}\times T_{2}).(3^{4}\mathpunct{:}(2^{2}\times\operatorname{SL}_{3}(3)))
(35)b(3^{5})_{b} 3A162B803{\rm A}_{162}{\rm B}_{80} 353^{5} 35.(34:Sp4(3).2)3^{5}.(3^{4}\mathpunct{:}\operatorname{Sp}_{4}(3).2)
\cdashline2-5 (34)a(3^{4})_{a} 3A52B26D23{\rm A}_{52}{\rm B}_{26}{\rm D}_{2} 33×GL2(K)3^{3}\times\operatorname{GL}_{2}(K) (33×GL2(K)).(SL3(3)×2)(3^{3}\times\operatorname{GL}_{2}(K)).(\operatorname{SL}_{3}(3)\times 2)
(34)b(3^{4})_{b} 3A54B263{\rm A}_{54}{\rm B}_{26} 33×(T2:3)3^{3}\times(T_{2}:3) (33×(T2:3)).(31+4:(2×GL2(3)))(3^{3}\times(T_{2}:3)).(3^{1+4}\mathpunct{:}(2\times\operatorname{GL}_{2}(3)))
(34)c(3^{4})_{c} 3B803{\rm B}_{80} 33×SL3(K)3^{3}\times\operatorname{SL}_{3}(K) (33×SL3(K)).(33:(2×SL3(3)))(3^{3}\times\operatorname{SL}_{3}(K)).(3^{3}:(2\times\operatorname{SL}_{3}(3)))
\cdashline2-5 (33)a(3^{3})_{a} 3A18B83{\rm A}_{18}{\rm B}_{8} 33×PSL3(K)3^{3}\times\operatorname{PSL}_{3}(K) (33×PSL3(K)).(32:GL2(3))(3^{3}\times\operatorname{PSL}_{3}(K)).(3^{2}\mathpunct{:}\operatorname{GL}_{2}(3))
(33)b(3^{3})_{b} 3B263{\rm B}_{26} 33×G2(K)3^{3}\times G_{2}(K) (33×G2(K)).SL3(3)(3^{3}\times G_{2}(K)).\operatorname{SL}_{3}(3)
Remark 6.2.

These remarks supplement Proposition 6.1.

  • (a)

    The normaliser structure is taken from [11, §8], which correct errors in [22] for the centralisers and normalisers of the non-toral subgroups 333^{3} in E7E_{7}, and (35)a(3^{5})_{a} and (33)b(3^{3})_{b} in E8E_{8}. Although we only give normaliser structure using short notation, in [11] the precise action of NG(E)/CG(E)N_{G}(E)/C_{G}(E) is given on each subgroup EE.

  • (b)

    For adjoint GG of type E6E_{6}, in [11, Theorem 8.10] the distribution is given of the pre-image E~\widetilde{E} of EE in the simply connected cover of GG. Since multiplication by an element of the centre permutes 3A3{\rm A}, 3B3{\rm B}, and elements whose square is in 3B3{\rm B} (while preserving the class of elements in 3C3{\rm C} and 3D3{\rm D}), it is straightforward to derive the above distribution of EE from that of E~\widetilde{E}, and vice-versa. The notation 3AB3{\rm AB} denotes the unique conjugacy class which is the image of the classes 3A3{\rm A} and 3B3{\rm B} (and also the inverse of elements in 3B3{\rm B}). The inverse of the class 3E3{\rm E} is denoted 3E3{\rm E}^{\prime}.

  • (c)

    For GG of type E7E_{7}, the classification is independent of the isogeny type, because the simply connected group has centre of order 22, and now the Schur-Zassenhaus Theorem implies that for p2p\neq 2 each elementary abelian pp-subgroup of the adjoint group lifts uniquely to an isomorphic copy in the simply connected group. In the table, the group ZZ is the kernel of the isogeny GscGG_{{\text{\rm sc}}}\to G from the simply connected cover GscG_{{\text{\rm sc}}} of GG, that is, Z=1Z=1 if G=GscG=G_{{\text{\rm sc}}}, and Z=2Z=2 if G=GadG=G_{{\text{\rm ad}}} and 2\ell\neq 2.

6.2. Statement of results for p=2p=2

We now consider elementary abelian 22-subgroups. Again, by Proposition 3.1 and Lemma 3.3 we are able to use results concerning complex Lie groups and compact real Lie groups, in particular [22] and [41]. However, in this case complete information is not given, and we supplement existing results with arguments for E7,scE_{7,{\text{\rm sc}}}, as well as our own normaliser structure calculations. Since the lists of subgroups for E8E_{8} and E7,adE_{7,{\text{\rm ad}}} are much larger than the other cases, we separate these out for readability. For the same reason, we have outsourced some more technical considerations to the appendix.

Proposition 6.3.

Let GG be a simple algebraic group of exceptional type over an algebraically closed field KK of characteristic 2\ell\neq 2. If EGE\leq G is a non-toral elementary abelian 22-subgroup, then (G,E)(G,E) appears in Table 5, Table 6, or Table 7. Each line of a table corresponds to a unique GG-conjugacy class of subgroups; supplementing comments are given in Remark 6.4.

Remark 6.4.

These remarks supplement Proposition 6.3.

  • (a)

    For GG of type E6E_{6}, the classification is independent of the isogeny type, because the simply connected group has centre of order 33 or 11, and the same argument as in Remark 6.2(c) applies. In the table, the group ZZ is the kernel of the isogeny GscGG_{{\text{\rm sc}}}\to G from the simply connected cover GscG_{{\text{\rm sc}}} of GG; thus, Z=1Z=1 if G=GscG=G_{{\text{\rm sc}}}, and Z=3Z=3 for G=GadG=G_{{\text{\rm ad}}} and 3\ell\neq 3.

  • (b)

    For GG adjoint of type E7E_{7}, the notation 2BC2{\rm BC} denotes the unique conjugacy class which is the image of the classes 2B2{\rm B} and 2C2{\rm C}. We abuse notation and write 4A4{\rm A} and 4H4{\rm H} for the involutions coming from the corresponding classes in the simply connected cover of GG.

  • (c)

    Since much of the information in Tables 6 and 7 is derived from [41, Sections 2–8], in the third column we give the name used in the classification there; we refer to Appendices A.1 and B.1 for further details. The notation for the centralisers in Tables 6 and 7 is as in [21].

The remainder of this section is devoted to a proof of Proposition 6.3. Using the algorithm of Section 5.1, we find that the number of classes of toral elementary abelian 22-subgroups is as given in Table 4.

Table 4. Number of classes of toral elementary abelian 22-subgroups, where the bracketed numbers count subgroups of order 202^{0}, 212^{1}, 222^{2}, etc.
GG G2G_{2} F4F_{4} E6E_{6} E7E_{7} E8E_{8}
Number (1,1,1)(1,1,1) (1,2,3,2,1)(1,2,3,2,1) (1,2,4,4,4,2,1)(1,2,4,4,4,2,1) (1,3,5,7,7,5,3,1)(1,3,5,7,7,5,3,1) (1,2,4,5,7,5,4,2,1)(1,2,4,5,7,5,4,2,1)
Total 33 99 1818 3232 3131
Table 5. Non-toral elementary abelian 22-subgroups of algebraic groups G2G_{2}, F4F_{4}, E6E_{6} and E7,scE_{7,{\text{\rm sc}}}.
𝑮\boldsymbol{G} 𝑬\boldsymbol{E} 𝐃𝐢𝐬𝐭(𝑬)\boldsymbol{\operatorname{Dist}(E)} 𝑪𝑮(𝑬)\boldsymbol{C_{G}(E)} 𝑵𝑮(𝑬)\boldsymbol{N_{G}(E)}
G2G_{2} 232^{3} 2A72{\rm A}_{7} 232^{3} 23.SL3(2)2^{3}.\operatorname{SL}_{3}(2)
F4F_{4} 252^{5} 2A28B32{\rm A}_{28}{\rm B}_{3} 252^{5} 25.(223).[SL3(2)×Sym3]2^{5}.(2^{2\cdot 3}).[\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3}]
\cdashline2-5 242^{4} 2A14B12{\rm A}_{14}{\rm B}_{1} 23×T1.22^{3}\times T_{1}.2 (23×T1.2).(23:SL3(2))(2^{3}\times T_{1}.2).(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))
\cdashline2-5 232^{3} 2A72{\rm A}_{7} 23×PGL2(K)2^{3}\times\operatorname{PGL}_{2}(K) (23:SL3(2))×PGL2(K)(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{PGL}_{2}(K)
E6E_{6} 252^{5} 2A28B32{\rm A}_{28}{\rm B}_{3} 23×T22^{3}\times T_{2} (23×T2).(223).(Sym3×SL3(2))(2^{3}\times T_{2}).(2^{2\cdot 3}).(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
\cdashline2-5 242^{4} 2A14B12{\rm A}_{14}{\rm B}_{1} 23×GL2(K)2^{3}\times\operatorname{GL}_{2}(K) (23×GL2(K)).(23:SL3(2))(2^{3}\times\operatorname{GL}_{2}(K)).(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))
\cdashline2-5 232^{3} 2A72{\rm A}_{7} 23×SL3(K)/Z2^{3}\times\operatorname{SL}_{3}(K)/Z (23:SL3(2))×SL3(K)/Z(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{SL}_{3}(K)/Z
E7,scE_{7,{\text{\rm sc}}} 262^{6} 2A1B31C312{\rm A}_{1}{\rm B}_{31}{\rm C}_{31} 23×SL2(K)32^{3}\times\operatorname{SL}_{2}(K)^{3} CG(E).223.(SL3(2)×Sym3)C_{G}(E).2^{2\cdot 3}.(\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3})
\cdashline2-5 (25)a(2^{5})_{a} 2A1B15C152{\rm A}_{1}{\rm B}_{15}{\rm C}_{15} 23×SL2(K)×Sp4(K)2^{3}\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K) CG(E).(23:SL3(2))C_{G}(E).(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))
(25)b(2^{5})_{b} 2B28C32{\rm B}_{28}{\rm C}_{3} 23×SL2(K)32^{3}\times\operatorname{SL}_{2}(K)^{3} CG(E).223.(SL3(2)×Sym3)C_{G}(E).2^{2\cdot 3}.(\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3})
(25)c(2^{5})_{c} 2B16C152{\rm B}_{16}{\rm C}_{15} 23×SL2(K)32^{3}\times\operatorname{SL}_{2}(K)^{3} CG(E).(2×(23:SL3(2)))C_{G}(E).(2\times(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)))
(25)d(2^{5})_{d} 2B12C192{\rm B}_{12}{\rm C}_{19} 23×SL2(K)32^{3}\times\operatorname{SL}_{2}(K)^{3} CG(E).(22+6:(Sym3×Sym3))C_{G}(E).(2^{2+6}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}))
\cdashline2-5 (24)a(2^{4})_{a} 2A1B7C72{\rm A}_{1}{\rm B}_{7}{\rm C}_{7} 23×Sp6(K)2^{3}\times\operatorname{Sp}_{6}(K) (23:SL3(2))×Sp6(K)(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{Sp}_{6}(K)
(24)b(2^{4})_{b} 2B14C12{\rm B}_{14}{\rm C}_{1} 23×SL2(K)×Sp4(K)2^{3}\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K) CG(E).(23:SL3(2))C_{G}(E).(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))
(24)c(2^{4})_{c} 2B8C72{\rm B}_{8}{\rm C}_{7} 23×SL2(K)×Sp4(K)2^{3}\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K) (23:SL3(2))×SL2(K)×Sp4(K)(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K)
(24)d(2^{4})_{d} 2B6C92{\rm B}_{6}{\rm C}_{9} 23×SL2(K)×Sp4(K)2^{3}\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K) CG(E).(2+1+4:Sym3)C_{G}(E).(2_{+}^{1+4}\mathpunct{:}\operatorname{Sym}_{3})
\cdashline2-5 (23)a(2^{3})_{a} 2B72{\rm B}_{7} 23×Sp6(K)2^{3}\times\operatorname{Sp}_{6}(K) (23:SL3(2))×Sp6(K)(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{Sp}_{6}(K)
(23)b(2^{3})_{b} 2B3C42{\rm B}_{3}{\rm C}_{4} 23×Sp6(K)2^{3}\times\operatorname{Sp}_{6}(K) (23:22.Sym3)×Sp6(K)(2^{3}\mathpunct{:}2^{2}.\operatorname{Sym}_{3})\times\operatorname{Sp}_{6}(K)
Table 6. Non-toral elementary abelian 22-subgroups of E7,adE_{7,{{\text{\rm ad}}}}, see Table 8 for more details on the normaliser quotient; here ZZ is the kernel of E7,scE7,adE_{7,{{\text{\rm sc}}}}\to E_{7,{{\text{\rm ad}}}}. The notation \leftrightarrow denotes an involution swapping two isomorphic simple subgroup factors. The subgroups listed in column labelled “UU” are used in Case (2) of the proof of Proposition 6.6.
𝑬\boldsymbol{E} 𝐃𝐢𝐬𝐭(𝑬)\boldsymbol{\operatorname{Dist}(E)} Name dim\dim 𝑼\boldsymbol{U} 𝑪𝑮(𝑬)\boldsymbol{C_{G}(E)} 𝑵𝑮(𝑬)/𝑪𝑮(𝑬)\boldsymbol{N_{G}(E)/C_{G}(E)}
282^{8} 2BC634A1644H282{\rm BC}_{63}4{\rm A}_{164}4{\rm H}_{28} F0,1,0,2F_{0,1,0,2} 0 F0,1,1,1F_{0,1,1,1} 282^{8} 27:SO7(2)2^{7}\mathpunct{:}\operatorname{SO}_{7}(2)
(27)a(2^{7})_{a} 2BC314A844H122{\rm BC}_{31}4{\rm A}_{84}4{\rm H}_{12} F2,3F_{2,3} 0 F1,3F_{1,3} 272^{7} (222×223):(Sym3×Sym3×SL3(2))(2^{2\cdot 2}\times 2^{2\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(27)b(2^{7})_{b} 2BC314A844H122{\rm BC}_{31}4{\rm A}_{84}4{\rm H}_{12} F0,1,1,1F_{0,1,1,1} 0 F0,1,0,1F_{0,1,0,1} 282^{8} (26:25):SO5(2)(2^{6}\mathpunct{:}2^{5})\mathpunct{:}\operatorname{SO}_{5}(2)
(27)c(2^{7})_{c} 2BC314A804H162{\rm BC}_{31}4{\rm A}_{80}4{\rm H}_{16} F1,0,0,2F_{1,0,0,2} 11 F1,2′′F_{1,2}^{\prime\prime} 26×T1.i2^{6}\times T_{1}.i (26:24):SO5(2)(2^{6}\mathpunct{:}2^{4})\mathpunct{:}\operatorname{SO}_{5}(2)
(27)d(2^{7})_{d} 2BC634A642{\rm BC}_{63}4{\rm A}_{64} F0,3′′F_{0,3}^{\prime\prime} 0 F1,2′′F_{1,2}^{\prime\prime} 282^{8} 26:Sp6(2)2^{6}\mathpunct{:}\operatorname{Sp}_{6}(2)
(26)a(2^{6})_{a} 2BC154A424H62{\rm BC}_{15}4{\rm A}_{42}4{\rm H}_{6} F1,3F_{1,3} 11 F0,3F_{0,3} 25×T1.i2^{5}\times T_{1}.i (22×23):(Sym3×SL3(2))(2^{2}\times 2^{3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(26)b(2^{6})_{b} 2BC154A364H122{\rm BC}_{15}4{\rm A}_{36}4{\rm H}_{12} F2,2F_{2,2} 44 F2,1F_{2,1} 22×T4.22^{2}\times T_{4}.2 (222×222):(Sym3×Sym3×Sym3)(2^{2\cdot 2}\times 2^{2\cdot 2})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(26)c(2^{6})_{c} 2BC314A284H42{\rm BC}_{31}4{\rm A}_{28}4{\rm H}_{4} F2,3F_{2,3}^{\prime} 33 F1,3F_{1,3}^{\prime} 23×T3.22^{3}\times T_{3}.2 (221×223):(Sym3×SL3(2))(2^{2\cdot 1}\times 2^{2\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(26)d(2^{6})_{d} 2BC154A384H102{\rm BC}_{15}4{\rm A}_{38}4{\rm H}_{10} F0,0,0,2F_{0,0,0,2} 33 F0,2′′F_{0,2}^{\prime\prime} 26×PSL2(K)2^{6}\times\operatorname{PSL}_{2}(K) 25:SO5(2)2^{5}\mathpunct{:}\operatorname{SO}_{5}(2)
(26)e(2^{6})_{e} 2BC154A424H62{\rm BC}_{15}4{\rm A}_{42}4{\rm H}_{6} F0,1,0,1F_{0,1,0,1} 11 F0,2′′F_{0,2}^{\prime\prime} 26×(T1.i)2^{6}\times(T_{1}.i) 25:SO5(2)2^{5}\mathpunct{:}\operatorname{SO}_{5}(2)
(26)f(2^{6})_{f} 2BC154A444H42{\rm BC}_{15}4{\rm A}_{44}4{\rm H}_{4} F0,1,2,0F_{0,1,2,0} 0 F1,0,2,0F_{1,0,2,0} 22×24.232^{2}\times 2^{4}.2^{3} (25:223):(Sym3×Sym3)(2^{5}\mathpunct{:}2^{2\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(26)g(2^{6})_{g} 2BC154A404H82{\rm BC}_{15}4{\rm A}_{40}4{\rm H}_{8} F1,0,1,1F_{1,0,1,1} 22 F0,0,1,1F_{0,0,1,1} 24×(T2.22)2^{4}\times(T_{2}.2^{2}) (25:24):(22:Sym3)(2^{5}\mathpunct{:}2^{4})\mathpunct{:}(2^{2}\mathpunct{:}\operatorname{Sym}_{3})
(26)h(2^{6})_{h} 2BC314A322{\rm BC}_{31}4{\rm A}_{32} F1,2′′F_{1,2}^{\prime\prime} 11 F0,2′′F_{0,2}^{\prime\prime} 26×(T1.i)2^{6}\times(T_{1}.i) (25:24):Sp4(2)(2^{5}\mathpunct{:}2^{4})\mathpunct{:}\operatorname{Sp}_{4}(2)
(25)a(2^{5})_{a} 2BC74A184H62{\rm BC}_{7}4{\rm A}_{18}4{\rm H}_{6} F1,2F_{1,2} 66 F1,1F_{1,1} 22×(T32SL2(K)).(i:1)2^{2}\times(T_{3}\circ_{2}\operatorname{SL}_{2}(K)).(i{:}1) (22×22):(Sym3×Sym3)(2^{2}\times 2^{2})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(25)b(2^{5})_{b} 2BC74A214H32{\rm BC}_{7}4{\rm A}_{21}4{\rm H}_{3} F0,3F_{0,3} 33 F0,2F_{0,2} 25×PGL2(K)2^{5}\times{\rm PGL}_{2}(K) Sym3×SL3(2)\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)
(25)c(2^{5})_{c} 2BC74A124H122{\rm BC}_{7}4{\rm A}_{12}4{\rm H}_{12} F2,1F_{2,1} 1212 F2,0F_{2,0} 22×(Spin4(K)2Spin4(K))2^{2}\times(\operatorname{Spin}_{4}(K)\circ_{2}\operatorname{Spin}_{4}(K)) (222×22):(Sym3×Sym3)(2^{2\cdot 2}\times 2^{2})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(25)d(2^{5})_{d} 2BC154A144H22{\rm BC}_{15}4{\rm A}_{14}4{\rm H}_{2} F1,3F_{1,3}^{\prime} 55 F0,3F_{0,3}^{\prime} 23×(T22SL2(K)).γ2^{3}\times(T_{2}\circ_{2}\operatorname{SL}_{2}(K)).\gamma (2×23):(SL3(2))(2\times 2^{3})\mathpunct{:}(\operatorname{SL}_{3}(2))
(25)e(2^{5})_{e} 2BC74A184H62{\rm BC}_{7}4{\rm A}_{18}4{\rm H}_{6} F0,0,1,1F_{0,0,1,1} 66 F0,0,0,1F_{0,0,0,1} 24×(SL2(K)2SL2(K)).2^{4}\times(\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)).\leftrightarrow (24:23):Sym3(2^{4}\mathpunct{:}2^{3})\mathpunct{:}\operatorname{Sym}_{3}
(25)f(2^{5})_{f} 2BC74A204H42{\rm BC}_{7}4{\rm A}_{20}4{\rm H}_{4} F1,0,2,0F_{1,0,2,0} 44 F2F_{2}^{\prime} 22×T4.232^{2}\times T_{4}.2^{3} (24:222):Sym3(2^{4}\mathpunct{:}2^{2\cdot 2})\mathpunct{:}\operatorname{Sym}_{3}
(25)g(2^{5})_{g} 2BC74A204H42{\rm BC}_{7}4{\rm A}_{20}4{\rm H}_{4} F1,0,0,1F_{1,0,0,1} 44 F0,0,0,1F_{0,0,0,1} 24×(GL2(K)/2).γ2^{4}\times(\operatorname{GL}_{2}(K)/2).\gamma (24:22):Sym3(2^{4}\mathpunct{:}2^{2})\mathpunct{:}\operatorname{Sym}_{3}
(25)h(2^{5})_{h} 2BC74A224H22{\rm BC}_{7}4{\rm A}_{22}4{\rm H}_{2} F0,1,1,0F_{0,1,1,0} 22 F0,1,0,0F_{0,1,0,0} 24×T2.D82^{4}\times T_{2}.D_{8} (24:23):Sym3(2^{4}\mathpunct{:}2^{3})\mathpunct{:}\operatorname{Sym}_{3}
(25)i(2^{5})_{i} 2BC154A162{\rm BC}_{15}4{\rm A}_{16} F2,1′′F_{2,1}^{\prime\prime} 33 F1,1′′F_{1,1}^{\prime\prime} 23×T3.232^{3}\times T_{3}.2^{3} (24:222):(Sym3×Sym3)(2^{4}\mathpunct{:}2^{2\cdot 2})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(25)j(2^{5})_{j} 2BC154A162{\rm BC}_{15}4{\rm A}_{16} F0,2′′F_{0,2}^{\prime\prime} 33 F1,1′′F_{1,1}^{\prime\prime} 26×PSL2(K)2^{6}\times\operatorname{PSL}_{2}(K) 24:Sp4(2)2^{4}\mathpunct{:}\operatorname{Sp}_{4}(2)
(25)k(2^{5})_{k} 2BC74A242{\rm BC}_{7}4{\rm A}_{24} F3F_{3}^{\prime} 0 F2F_{2}^{\prime} 22×23+62^{2}\times 2^{3+6} 232:(SL3(2)×Sym3)2^{3\cdot 2}\mathpunct{:}(\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3})
(25)l(2^{5})_{l} 2BC312{\rm BC}_{31} F2′′F_{2}^{\prime\prime} 99 F1′′F_{1}^{\prime\prime} 23×SL2(K)2(SL2(K))22^{3}\times\operatorname{SL}_{2}(K)\circ_{2}(\operatorname{SL}_{2}(K))^{2} 223:(Sym3×SL3(2))2^{2\cdot 3}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(24)a(2^{4})_{a} 2BC34A94H32{\rm BC}_{3}4{\rm A}_{9}4{\rm H}_{3} F0,2F_{0,2} 1010 F0,1F_{0,1} 22×(T23SL3(K)).(i:γ)2^{2}\times(T_{2}\circ_{3}\operatorname{SL}_{3}(K)).(i{:}\gamma) Sym3×Sym3\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}
(24)b(2^{4})_{b} 2BC34A64H62{\rm BC}_{3}4{\rm A}_{6}4{\rm H}_{6} F1,1F_{1,1} 1616 F0,1F_{0,1} 22×(SL2(K)22Sp4(K))2^{2}\times(\operatorname{SL}_{2}(K)^{2}\circ_{2}\operatorname{Sp}_{4}(K)) (22×2):Sym3(2^{2}\times 2)\mathpunct{:}\operatorname{Sym}_{3}
(24)c(2^{4})_{c} 2BC34H122{\rm BC}_{3}4{\rm H}_{12} F2,0F_{2,0} 2828 F1,0F_{1,0} 22×Spin8(K)2^{2}\times\operatorname{Spin}_{8}(K) 222:(Sym3×Sym3)2^{2\cdot 2}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(24)d(2^{4})_{d} 2BC74A74H12{\rm BC}_{7}4{\rm A}_{7}4{\rm H}_{1} F0,3F_{0,3}^{\prime} 99 F0′′F_{0}^{\prime\prime} 23×(GL3(K)/2).γ2^{3}\times(\operatorname{GL}_{3}(K)/2).\gamma SL3(2)\operatorname{SL}_{3}(2)
(24)e(2^{4})_{e} 2BC34A84H42{\rm BC}_{3}4{\rm A}_{8}4{\rm H}_{4} F0,0,2,0F_{0,0,2,0} 1212 F0,0,1,0F_{0,0,1,0} 22×((SL2(K))22(SL2(K))2).222^{2}\times((\operatorname{SL}_{2}(K))^{2}\circ_{2}(\operatorname{SL}_{2}(K))^{2}).2^{2} (23:22):Sym3(2^{3}\mathpunct{:}2^{2})\mathpunct{:}\operatorname{Sym}_{3}
(24)f(2^{4})_{f} 2BC34A94H32{\rm BC}_{3}4{\rm A}_{9}4{\rm H}_{3} F0,0,0,1F_{0,0,0,1} 1010 F0,1′′F_{0,1}^{\prime\prime} 24×PSp4(K)2^{4}\times\operatorname{PSp}_{4}(K) 23:Sym32^{3}\mathpunct{:}\operatorname{Sym}_{3}
(24)g(2^{4})_{g} 2BC34A114H12{\rm BC}_{3}4{\rm A}_{11}4{\rm H}_{1} F0,1,0,0F_{0,1,0,0} 66 F0,1′′F_{0,1}^{\prime\prime} 24×(PSL2(K))2.2^{4}\times(\operatorname{PSL}_{2}(K))^{2}.\leftrightarrow 23:Sym32^{3}\mathpunct{:}\operatorname{Sym}_{3}
(24)h(2^{4})_{h} 2BC34A104H22{\rm BC}_{3}4{\rm A}_{10}4{\rm H}_{2} F1,0,1,0F_{1,0,1,0} 88 F1,0,0,0F_{1,0,0,0} 22×(GL2(K)2GL2(K)).222^{2}\times(\operatorname{GL}_{2}(K)\circ_{2}\operatorname{GL}_{2}(K)).2^{2} 23:222^{3}\mathpunct{:}2^{2}
(24)i(2^{4})_{i} 2BC74A82{\rm BC}_{7}4{\rm A}_{8} F1,1′′F_{1,1}^{\prime\prime} 77 F0,1′′F_{0,1}^{\prime\prime} 23×((T1.i)2SO4(K)).(i:γ)2^{3}\times((T_{1}.i)\circ_{2}\operatorname{SO}_{4}(K)).(i{:}\gamma) (23:22):Sym3(2^{3}\mathpunct{:}2^{2})\mathpunct{:}\operatorname{Sym}_{3}
(24)j(2^{4})_{j} 2BC34A122{\rm BC}_{3}4{\rm A}_{12} F2F_{2}^{\prime} 44 F1F_{1}^{\prime} 22×T4.2+1+42^{2}\times T_{4}.2_{+}^{1+4} 222:(Sym3×Sym3)2^{2\cdot 2}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3})
(24)k(2^{4})_{k} 2BC152{\rm BC}_{15} F1′′F_{1}^{\prime\prime} 1313 F0′′F_{0}^{\prime\prime} 23×SL2(K)2Sp4(K)2^{3}\times\operatorname{SL}_{2}(K)\circ_{2}\operatorname{Sp}_{4}(K) 23:SL3(2)2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)
(23)a(2^{3})_{a} 2BC14A34H32{\rm BC}_{1}4{\rm A}_{3}4{\rm H}_{3} F0,1F_{0,1} 2424 F0,0,0,0F_{0,0,0,0} 22×SL2(K)2Sp6(K)2^{2}\times\operatorname{SL}_{2}(K)\circ_{2}\operatorname{Sp}_{6}(K) Sym3\operatorname{Sym}_{3}
(23)b(2^{3})_{b} 2BC14H62{\rm BC}_{1}4{\rm H}_{6} F1,0F_{1,0} 3636 F0,0F_{0,0} 22×Spin9(K)2^{2}\times\operatorname{Spin}_{9}(K) 22:Sym32^{2}\mathpunct{:}\operatorname{Sym}_{3}
(23)c(2^{3})_{c} 2BC14A54H12{\rm BC}_{1}4{\rm A}_{5}4{\rm H}_{1} F1,0,0,0F_{1,0,0,0} 1616 F0,0,0,0F_{0,0,0,0} 22×(GL4(K)/Z).γ2^{2}\times(\operatorname{GL}_{4}(K)/Z).\gamma 222^{2}
(23)d(2^{3})_{d} 2BC14A44H22{\rm BC}_{1}4{\rm A}_{4}4{\rm H}_{2} F0,0,1,0F_{0,0,1,0} 2020 F0,0,0,0F_{0,0,0,0} 22×(Sp4(K)2Sp4(K)).2^{2}\times(\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K)).\leftrightarrow 22:22^{2}\mathpunct{:}2
(23)e(2^{3})_{e} 2BC34A42{\rm BC}_{3}4{\rm A}_{4} F0,1′′F_{0,1}^{\prime\prime} 1515 23×PSO6(K).γ2^{3}\times\operatorname{PSO}_{6}(K).\gamma 22:Sym32^{2}\mathpunct{:}\operatorname{Sym}_{3}
(23)f(2^{3})_{f} 2BC14A62{\rm BC}_{1}4{\rm A}_{6} F1F_{1}^{\prime} 1212 F0F_{0}^{\prime} 22×(SO4(K)2SO4(K)).γ:γ,2^{2}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K)).\langle\gamma{:}\gamma,\leftrightarrow\rangle 22:Sym32^{2}\mathpunct{:}\operatorname{Sym}_{3}
(23)g(2^{3})_{g} 2BC72{\rm BC}_{7} F0′′F_{0}^{\prime\prime} 2121 23×PSp6(K)2^{3}\times\text{PSp}_{6}(K) SL3(2)\operatorname{SL}_{3}(2)
(22)a(2^{2})_{a} 4H34{\rm H}_{3} F0,0F_{0,0} 5252 22×F4(K)2^{2}\times F_{4}(K) Sym3\operatorname{Sym}_{3}
(22)b(2^{2})_{b} 4A2H14{\rm A}_{2}{\rm H}_{1} F0,0,0,0F_{0,0,0,0} 3636 22×PSp8(K)2^{2}\times\operatorname{PSp}_{8}(K) 22
(22)c(2^{2})_{c} 4A34{\rm A}_{3} F0F_{0}^{\prime} 2828 22×PΩ8(K)2^{2}\times\operatorname{P\Omega}_{8}(K) Sym3\operatorname{Sym}_{3}
Table 7. Non-toral elementary abelian 22-subgroups of the algebraic group G=E8G=E_{8}; here L=E7,adGL=E_{7,{\text{\rm ad}}}\leq G and the subgroup given in the column labelled “XLX\leq L” is from Table 6 and used in Section 6.8.
𝑬\boldsymbol{E} 𝐃𝐢𝐬𝐭(𝐄)\boldsymbol{\rm{Dist}(E)} Name dim\dim XLX\leq L 𝑪𝑮(𝑬)\boldsymbol{C_{G}(E)} 𝑵𝑮(𝑬)/𝑪𝑮(𝑬)\boldsymbol{N_{G}(E)/C_{G}(E)}
292^{9} 2A120B3912{\rm A}_{120}{\rm B}_{391} F0,1,0,2F_{0,1,0,2} 0 F0,1,0,2F_{0,1,0,2} 292^{9} 28:SO8+(2)2^{8}\mathpunct{:}\operatorname{SO}_{8}^{+}(2)
(28)a(2^{8})_{a} 2A56B1992{\rm A}_{56}{\rm B}_{199} F2,3F_{2,3} 0 F2,3F_{2,3} 282^{8} 226:(Sym3×(SL3(2)2))2^{2\cdot 6}\mathpunct{:}(\operatorname{Sym}_{3}\times(\operatorname{SL}_{3}(2)\wr 2))
(28)b(2^{8})_{b} 2A56B1992{\rm A}_{56}{\rm B}_{199} F0,1,1,1F_{0,1,1,1} 0 F0,1,1,1F_{0,1,1,1} 292^{9} (2×26):(26:(SO6+(2)))(2\times 2^{6})\mathpunct{:}(2^{6}\mathpunct{:}(\operatorname{SO}_{6}^{+}(2)))
(28)c(2^{8})_{c} 2A64B1912{\rm A}_{64}{\rm B}_{191} F1,0,0,2F_{1,0,0,2} 11 F1,0,0,2F_{1,0,0,2} 27×T1.22^{7}\times T_{1}.2 27:SO7(2)2^{7}\mathpunct{:}\operatorname{SO}_{7}(2)
(27)a(2^{7})_{a} 2A40B872{\rm A}_{40}{\rm B}_{87} F2,2F_{2,2} 44 F2,2F_{2,2} 23×T4.22^{3}\times T_{4}.2 (2221×2213):(Sym3×Sym3×SL3(2))(2^{2\cdot 2\cdot 1}\times 2^{2\cdot 1\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(27)b(2^{7})_{b} 2A28B992{\rm A}_{28}{\rm B}_{99} F1,3F_{1,3} 11 F1,3F_{1,3} 26×T1.22^{6}\times T_{1}.2 26:(SL3(2)2)2^{6}\mathpunct{:}(\operatorname{SL}_{3}(2)\wr 2)
(27)c(2^{7})_{c} 2A24B1032{\rm A}_{24}{\rm B}_{103} F0,1,2,0F_{0,1,2,0} 0 F0,1,2,0F_{0,1,2,0} 23×24.232^{3}\times 2^{4}.2^{3} (22×24):(224:(Sym3×SO4+(2)))(2^{2}\times 2^{4})\mathpunct{:}(2^{2\cdot 4}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SO}_{4}^{+}(2)))
(27)d(2^{7})_{d} 2A28B992{\rm A}_{28}{\rm B}_{99} F0,1,0,1F_{0,1,0,1} 11 F0,1,0,1F_{0,1,0,1} 27×T1.22^{7}\times T_{1}.2 26:SO6+(2)2^{6}\mathpunct{:}\operatorname{SO}_{6}^{+}(2)
(27)e(2^{7})_{e} 2A32B952{\rm A}_{32}{\rm B}_{95} F1,0,1,1F_{1,0,1,1} 22 F1,0,1,1F_{1,0,1,1} 25×T2.222^{5}\times T_{2}.2^{2} (2×25):(25:SO5(2))(2\times 2^{5})\mathpunct{:}(2^{5}\mathpunct{:}\operatorname{SO}_{5}(2))
(27)f(2^{7})_{f} 2A36B912{\rm A}_{36}{\rm B}_{91} F0,0,0,2F_{0,0,0,2} 33 F0,0,0,2F_{0,0,0,2} 27×PSL2(K)2^{7}\times{\rm PSL}_{2}(K) 26:SO6(2)2^{6}\mathpunct{:}\operatorname{SO}_{6}^{-}(2)
(26)a(2^{6})_{a} 2A32B312{\rm A}_{32}{\rm B}_{31} F2,1F_{2,1} 1212 F2,1F_{2,1} 23×(SL2(K)2)2(SL2(K)2){2^{3}}\times(\operatorname{SL}_{2}(K)^{2})\circ_{2}(\operatorname{SL}_{2}(K)^{2}) (221×223):(Sym3×SL3(2))(2^{2\cdot 1}\times 2^{2\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(26)b(2^{6})_{b} 2A20B432{\rm A}_{20}{\rm B}_{43} F1,2F_{1,2} 66 F1,2F_{1,2} 23×(T32SL2(K)).22^{3}\times(T_{3}\circ_{2}\operatorname{SL}_{2}(K)).2 (221×213):(Sym3×SL3(2))(2^{2\cdot 1}\times 2^{1\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(26)c(2^{6})_{c} 2A14B492{\rm A}_{14}{\rm B}_{49} F0,3F_{0,3} 33 F0,3F_{0,3} 26×PGL2(K)2^{6}\times{\rm PGL}_{2}(K) SL3(2)2\operatorname{SL}_{3}(2)\wr 2
(26)d(2^{6})_{d} 2A12B512{\rm A}_{12}{\rm B}_{51} F0,1,1,0F_{0,1,1,0} 22 F0,1,1,0F_{0,1,1,0} 25×T2.D82^{5}\times T_{2}.D_{8} (2×24):(24:(SO4+(2)))(2\times 2^{4})\mathpunct{:}(2^{4}\mathpunct{:}(\operatorname{SO}_{4}^{+}(2)))
(26)e(2^{6})_{e} 2A16B472{\rm A}_{16}{\rm B}_{47} F1,0,2,0F_{1,0,2,0} 44 F1,0,2,0F_{1,0,2,0} 23×T4.232^{3}\times T_{4}.2^{3} (22×23):(223:(Sym3×SO3(2)))(2^{2}\times 2^{3})\mathpunct{:}(2^{2\cdot 3}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SO}_{3}(2)))
(26)f(2^{6})_{f} 2A16B472{\rm A}_{16}{\rm B}_{47} F1,0,0,1F_{1,0,0,1} 44 F1,0,0,1F_{1,0,0,1} 25×(GL2(K)/2).22^{5}\times({\rm GL}_{2}(K)/2).2 25:SO5(2)2^{5}\mathpunct{:}\operatorname{SO}_{5}(2)
(26)g(2^{6})_{g} 2A20B432{\rm A}_{20}{\rm B}_{43} F0,0,1,1F_{0,0,1,1} 66 F0,0,1,1F_{0,0,1,1} 25×(SL2(K)2SL2(K)).22^{5}\times(\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)).2 (2×24):(24:(SO4(2)))(2\times 2^{4})\mathpunct{:}(2^{4}\mathpunct{:}(\operatorname{SO}_{4}^{-}(2)))
(26)h(2^{6})_{h} 2A8B552{\rm A}_{8}{\rm B}_{55} F3,2′′F_{3,2}^{\prime\prime} 0 F3F_{3}^{\prime} 23×23+62^{3}\times 2^{3+6} 232:((23×22):(SL3(2)×Sym3))2^{3\cdot 2}\mathpunct{:}((2^{3}\times 2^{2})\mathpunct{:}(\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3}))
(25)a(2^{5})_{a} 2A28B32{\rm A}_{28}{\rm B}_{3} F2,0F_{2,0} 2828 F2,0F_{2,0} 23×Spin8(K)2^{3}\times\operatorname{Spin}_{8}(K) 223:(Sym3×SL3(2))2^{2\cdot 3}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2))
(25)b(2^{5})_{b} 2A16B152{\rm A}_{16}{\rm B}_{15} F1,1F_{1,1} 1616 F1,1F_{1,1} 23×(SL2(K)22Sp4(K))2^{3}\times(\operatorname{SL}_{2}(K)^{2}\circ_{2}\operatorname{Sp}_{4}(K)) 2×23:SL3(2)2\times 2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)
(25)c(2^{5})_{c} 2A10B212{\rm A}_{10}{\rm B}_{21} F0,2F_{0,2} 1010 F0,2F_{0,2} 23×(T1×GL3(K)).22^{3}\times(T_{1}\times\operatorname{GL}_{3}(K)).2 Sym3×SL3(2)\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)
(25)d(2^{5})_{d} 2A6B252{\rm A}_{6}{\rm B}_{25} F0,1,0,0F_{0,1,0,0} 66 F0,1,0,0F_{0,1,0,0} 25×PSL2(K)2.22^{5}\times{{\rm PSL}_{2}(K)^{2}}.2 24:SO4+(2)2^{4}\mathpunct{:}\operatorname{SO}_{4}^{+}(2)
(25)e(2^{5})_{e} 2A8B232{\rm A}_{8}{\rm B}_{23} F1,0,1,0F_{1,0,1,0} 88 F1,0,1,0F_{1,0,1,0} 23×(T222(SL2(K)2)).222^{3}\times(T_{2}\circ_{2^{2}}(\operatorname{SL}_{2}(K)^{2})).2^{2} (2×23):(23:(SO3(2)))(2\times 2^{3})\mathpunct{:}(2^{3}\mathpunct{:}(\operatorname{SO}_{3}(2)))
(25)f(2^{5})_{f} 2A12B192{\rm A}_{12}{\rm B}_{19} F0,0,2,0F_{0,0,2,0} 1212 F0,0,2,0F_{0,0,2,0} 23×((SL2(K)2)2(SL2(K)2)).222^{3}\times((\operatorname{SL}_{2}(K)^{2})\circ_{2}(\operatorname{SL}_{2}(K)^{2})).2^{2} (22×22):(222:(Sym3×Sym3))(2^{2}\times 2^{2})\mathpunct{:}(2^{2\cdot 2}\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}))
(25)g(2^{5})_{g} 2A10B212{\rm A}_{10}{\rm B}_{21} F0,0,0,1F_{0,0,0,1} 1010 F0,0,0,1F_{0,0,0,1} 25×PSp4(K)2^{5}\times{\rm PSp}_{4}(K) 24:(SO4(2))2^{4}\mathpunct{:}(\operatorname{SO}_{4}^{-}(2))
(25)h(2^{5})_{h} 2A4B272{\rm A}_{4}{\rm B}_{27} F2,2′′F_{2,2}^{\prime\prime} 44 F2F_{2}^{\prime} 23×T4.2+1+4{2^{3}}\times T_{4}.2_{+}^{1+4} 222:((22×22):(Sym3×Sym3))2^{2\cdot 2}\mathpunct{:}((2^{2}\times 2^{2})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}))
(25)i(2^{5})_{i} 2B312{\rm B}_{31} F5F_{5}^{\prime} 0 25+102^{5+10} SL5(2)\operatorname{SL}_{5}(2)
(24)a(2^{4})_{a} 2A14B12{\rm A}_{14}{\rm B}_{1} F1,0F_{1,0} 3636 F1,0F_{1,0} 23×Spin9(K)2^{3}\times\operatorname{Spin}_{9}(K) 23:SL3(2)2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)
(24)b(2^{4})_{b} 2A8B72{\rm A}_{8}{\rm B}_{7} F0,1F_{0,1} 2424 F0,1F_{0,1} 23×SL2(K)2Sp6(K)2^{3}\times\operatorname{SL}_{2}(K)\circ_{2}\operatorname{Sp}_{6}(K) SL3(2)\operatorname{SL}_{3}(2)
(24)c(2^{4})_{c} 2A4B112{\rm A}_{4}{\rm B}_{11} F1,0,0,0F_{1,0,0,0} 1616 F1,0,0,0F_{1,0,0,0} 23×(GL4(K)/2).22^{3}\times(\operatorname{GL}_{4}(K)/2).2 23:SO3(2)2^{3}\mathpunct{:}\operatorname{SO}_{3}(2)
(24)d(2^{4})_{d} 2A6B92{\rm A}_{6}{\rm B}_{9} F0,0,1,0F_{0,0,1,0} 2020 F0,0,1,0F_{0,0,1,0} 23×(Sp4(K)2Sp4(K)).22^{3}\times(\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K)).2 23:(22:Sym3)2^{3}\mathpunct{:}(2^{2}\mathpunct{:}\operatorname{Sym}_{3})
(24)e(2^{4})_{e} 2A2B132{\rm A}_{2}{\rm B}_{13} F1,2′′F_{1,2}^{\prime\prime} 1212 F1F_{1}^{\prime} 23×(SO4(K)2SO4(K)).222^{3}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K)).2^{2} 212:((2×22):Sym3)2^{1\cdot 2}\mathpunct{:}((2\times 2^{2})\mathpunct{:}\operatorname{Sym}_{3})
(23)a(2^{3})_{a} 2A72{\rm A}_{7} F0,0F_{0,0} 5252 F0,0F_{0,0} 23×F4(K)2^{3}\times F_{4}(K) SL3(2)\operatorname{SL}_{3}(2)
(23)b(2^{3})_{b} 2A3B42{\rm A}_{3}{\rm B}_{4} F0,0,0,0F_{0,0,0,0} 3636 F0,0,0,0F_{0,0,0,0} 23×PSp8(K)2^{3}\times{\rm P}\operatorname{Sp}_{8}(K) 22:Sym32^{2}\mathpunct{:}\operatorname{Sym}_{3}
(23)c(2^{3})_{c} 2A1B62{\rm A}_{1}{\rm B}_{6} F0,2′′F_{0,2}^{\prime\prime} 2828 F0F_{0}^{\prime} 23×PΩ8(K)2^{3}\times{\rm P}\Omega_{8}(K) 22:Sym32^{2}\mathpunct{:}\operatorname{Sym}_{3}

It follows from our description in Section 5.1 that the number of toral subgroups does not depend on the isogeny type (although the class distributions and normaliser structure of the subgroups do vary). On the other hand, [41, Theorem 1.1] tells us that for a group GG of type G2G_{2}, F4F_{4}, E6E_{6}, E7E_{7}, and E8E_{8} we respectively have exactly 44, 1212, 5151, 7878, and 6666 classes of elementary abelian 22-subgroups in Aut(Lie(G))\operatorname{Aut}(\operatorname{Lie}(G)). If GG is adjoint, then G=Aut(Lie(G))G=\operatorname{Aut}(\operatorname{Lie}(G)), unless GG has type E6E_{6} in which case (by inspecting [41, §3.4]) we see that G=Aut(Lie(G))G=\operatorname{Aut}(\operatorname{Lie}(G))^{\circ} contains 2121 classes of elementary abelian 22-subgroups; using the notation of [41], these are the classes in ‘Class 3’ and ‘Class 4’.

Thus for adjoint groups of type G2G_{2}, F4F_{4}, E6E_{6}, E7E_{7}, and E8E_{8} there are respectively 11, 33, 33, 4646, and 3535 classes of non-toral elementary abelian 22-subgroups. So if we verify the information stated in the tables, it becomes evident that all the listed subgroups are non-conjugate, and counting then shows that these are all non-toral subgroups with elementary abelian image in G/Z(G)G/Z(G). For the simply connected group E7,scE_{7,{\text{\rm sc}}}, which is not isomorphic to its adjoint version as the characteristic is not 22, we provide our own detailed calculations, showing explicitly that the 1111 given classes of subgroups above constitute all non-toral subgroups.

We now split the proof into several cases.

6.3. Proof of Proposition 6.3 for G=G2(K)G=G_{2}(K).

This follows from [22, Table I].

6.4. Proof of Proposition 6.3 for G=F4(K)G=F_{4}(K).

The collection of all elementary abelian 22-subgroups of GG is described in [41, Proposition 5.2]. These twelve subgroups are labelled Fr,sF_{r,s} for r2r\leq 2 and s3s\leq 3, and it follows directly from the proof of [loc. cit.] that the class distribution of Fr,sF_{r,s} is 2A2r+s2r2B2r12{\rm A}_{2^{r+s}-2^{r}-2}{\rm B}_{2^{r}-1}. Using our algorithm from Section 5.1, we find that 99 of these 1212 possible class distributions are the distribution of a toral elementary abelian 22-subgroup; the exceptions are 2A28B3=Dist(F2,3)2{\rm A}_{28}{\rm B}_{3}=\operatorname{Dist}(F_{2,3}), 2A14B1=Dist(F1,3)2{\rm A}_{14}{\rm B}_{1}=\operatorname{Dist}(F_{1,3}), and 2A7=Dist(F0,3)2{\rm A}_{7}=\operatorname{Dist}(F_{0,3}). We conclude that GG has exactly three conjugacy classes of non-toral subgroups (cf. also [22, Table I and Theorem 7.3]).

The structure of NG(Fr,s)/CG(Fr,s)N_{G}(F_{r,s})/C_{G}(F_{r,s}) for each subgroup occurring is given in [41, Proposition 5.5]; it remains to consider their centralisers. Using Lemma 3.5, the subgroups of order 232^{3}, 242^{4}, and 252^{5} have centralisers of dimension 33, 11, and 0, respectively. By [31, Theorem 1], the group GG has a maximal connected subgroup of type A1G2A_{1}G_{2}, where the factor A1A_{1} is adjoint as this maximal subgroup is not contained in an involution centraliser in GG. The non-toral subgroup E=23E=2^{3} of this G2G_{2} factor, having all involutions conjugate, must be non-toral in GG. Thus EE is a representative of the GG-class of non-toral subgroups 232^{3}. Now EE centralises a subgroup A1A_{1}, and we deduce that CG(E)PGL2(K)C_{G}(E)^{\circ}\cong\operatorname{PGL}_{2}(K). Moreover, CG(E)C_{G}(E) normalises CG(E)C_{G}(E)^{\circ}; since the latter has no outer automorphisms, CG(E)PGL2(K)CG(PGL2(K))C_{G}(E)\leq\operatorname{PGL}_{2}(K)C_{G}(\operatorname{PGL}_{2}(K)). From the maximality of the subgroup of type A1G2A_{1}G_{2} it follows that CG(PGL2(K))=G2(K)C_{G}(\operatorname{PGL}_{2}(K))=G_{2}(K), hence CG(E)PGL2(K)G2(K)C_{G}(E)\leq\operatorname{PGL}_{2}(K)G_{2}(K). Since E<G2(K)E<G_{2}(K) is the unique non-toral subgroup and CG2(K)(E)=EC_{G_{2}(K)}(E)=E, we have CG(E)=E×PGL2(K)C_{G}(E)=E\times\operatorname{PGL}_{2}(K).

If EE is non-toral of order 242^{4}, then CG(E)C_{G}(E) is the centraliser of a non-central involution of 23×PGL2(K)2^{3}\times\operatorname{PGL}_{2}(K), and is therefore 23×(T1:2)2^{3}\times(T_{1}\mathpunct{:}2). Finally, when EE is non-toral of order 252^{5} we have ECG(E)C23×(T1:2)(E)=23×(22)=EE\leq C_{G}(E)\leq C_{2^{3}\times(T_{1}\mathpunct{:}2)}(E)=2^{3}\times(2^{2})=E.

6.5. Proof of Proposition 6.3 for G=E6(K)G=E_{6}(K).

Recall that ZZ is the kernel of the isogeny from the simply connected cover of GG. From [22, Table I] it follows that, up to conjugacy, the three non-toral subgroups of the simply connected group of type E6E_{6} are precisely the images of the non-toral subgroups of F4(K)F_{4}(K) under the inclusion F4(K)E6,sc(K)F_{4}(K)\to E_{6,{\text{\rm sc}}}(K): in the terminology of [22], this is because these are each precisely the subgroups of complexity at least 3. Their class distributions in Table 5 follow from their distributions in F4(K)F_{4}(K). Using Lemma 3.5, the centralisers of E=23E=2^{3}, 242^{4}, and 252^{5} have dimension 88, 44, and 22, respectively. By [22, Remark 8.3], the group GG has a maximal subgroup MM of type A2G2A_{2}G_{2}. The unique non-toral 23G22^{3}\leq G_{2} is non-toral in GG (since all its involutions are conjugate), and extends to a non-toral 25G2^{5}\leq G contained in MM. The known dimension tells us that CG(23)C_{G}(2^{3})^{\circ} is precisely the factor of type A2A_{2}. We claim that its centre is Z(Gsc)/ZZ(G_{{\text{\rm sc}}})/Z. It follows from [31, Tables 10.1 and 10.2] that this factor A2A_{2} has a natural 33-dimensional module (highest weight ‘1010’) as a composition factor of the 2727-dimensional module, hence this factor A2A_{2} has a non-trivial centre when GG is simply connected; on the other hand, all composition factors of this subgroup A2A_{2} on L(G)L(G) have highest weight ‘1111’ or ‘0000’, hence occur as sub-quotients of 100110\otimes 01. Thus the centre of this subgroup A2A_{2} acts trivially on L(G)L(G), and so lies in ker(GGad)=Z(Gsc)/Z\ker(G\to G_{{\text{\rm ad}}})=Z(G_{{\text{\rm sc}}})/Z. Since MM is maximal, the normaliser of CG(23)C_{G}(2^{3})^{\circ} in GG is MM, hence CG(23)MC_{G}(2^{3})\leq M. Since MM is a direct product and 23<G22^{3}<G_{2}, we have

CG(23)=SL3(K)/Z×CG2(K)(23)=23×SL3(K)/Z.C_{G}(2^{3})=\operatorname{SL}_{3}(K)/Z\times C_{G_{2}(K)}(2^{3})=2^{3}\times\operatorname{SL}_{3}(K)/Z.

Since CG(25)CG(24)CG(23)=23×SL3(K)/ZC_{G}(2^{5})\leq C_{G}(2^{4})\leq C_{G}(2^{3})=2^{3}\times\operatorname{SL}_{3}(K)/Z, we observe that CG(24)C_{G}(2^{4})^{\circ} is a 44-dimensional reductive subgroup of SL3(K)/Z\operatorname{SL}_{3}(K)/Z, and is therefore a Levi subgroup isomorphic to GL2(K)\operatorname{GL}_{2}(K). The centraliser CG(24)C_{G}(2^{4}) normalises this GL2(K)\operatorname{GL}_{2}(K), hence is equal to 23×GL2(K)2^{3}\times\operatorname{GL}_{2}(K). Next, CG(25)C_{G}(2^{5})^{\circ} is reductive and 22-dimensional, hence is a subtorus of the subgroup GL2(K)\operatorname{GL}_{2}(K) above. The centraliser CG(25)C_{G}(2^{5}) is contained in 23×GL2(K)2^{3}\times\operatorname{GL}_{2}(K) and normalises this torus, hence is the product of 232^{3} with an elementary abelian subgroup of GL2(K)\operatorname{GL}_{2}(K). Every such subgroup is toral in GL2(K)\operatorname{GL}_{2}(K) by [32, Corollary 14.17], hence CG(25)=23×T2C_{G}(2^{5})=2^{3}\times T_{2}.

Finally, the groups NG(E)/CG(E)N_{G}(E)/C_{G}(E) are given in [41, Proposition 6.10], but we correct errors for 252^{5} and 242^{4}. Note that the three non-toral groups are F0,3F_{0,3}, F1,3F_{1,3}, and F2,3F_{2,3} as defined in [41, p. 272], see also Case F4F_{4} above. Since 25F4(K)G2^{5}\leq F_{4}(K)\leq G and OutF4(K)(25)=223.(Sym3×SL3(2))\operatorname{Out}_{F_{4}(K)}(2^{5})=2^{2\cdot 3}.(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)), we have OutG(25)223.(Sym3×SL3(2))\operatorname{Out}_{G}(2^{5})\geq 2^{2\cdot 3}.(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)). Note that E=25E=2^{5} contains involutions 2A2{\rm A} and 2B2{\rm B}, so OutG(25)\operatorname{Out}_{G}(2^{5}) is a proper subgroup of Out(25)=SL5(2)\operatorname{Out}(2^{5})=\operatorname{SL}_{5}(2). But 223.(Sym3×SL3(2))2^{2\cdot 3}.(\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)) is a maximal (parabolic) subgroup of Out(25)\operatorname{Out}(2^{5}), so OutG(25)=OutF4(K)(25)\operatorname{Out}_{G}(2^{5})=\operatorname{Out}_{F_{4}(K)}(2^{5}). Similarly, NG(24)=(23×GL2(K))(23:SL3(2))N_{G}(2^{4})=(2^{3}\times\operatorname{GL}_{2}(K))(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)), since OutF4(K)(24)=23:SL3(2)Out(24)=SL4(2)\operatorname{Out}_{F_{4}(K)}(2^{4})=2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)\leq\operatorname{Out}(2^{4})=\operatorname{SL}_{4}(2) is maximal.

6.6. Proof of Proposition 6.3 for G=E7,sc(K)G=E_{7,{{\text{\rm sc}}}}(K).

By [22, Table I] there exists a unique maximal non-toral subgroup M=26M=2^{6} of GG with

CG(M)=23×SL2(K)3andNG(M)/CG(M)=223.(SL3(2)×Sym3).C_{G}(M)=2^{3}\times\operatorname{SL}_{2}(K)^{3}\quad\text{and}\quad N_{G}(M)/C_{G}(M)=2^{2\cdot 3}.(\operatorname{SL}_{3}(2)\times\operatorname{Sym}_{3}).

We now determine a set of generators for MM which allow us to easily determine the class of an element of MM, and to concretely realise NG(M)/CG(M)N_{G}(M)/C_{G}(M) as the subgroup of GL6(2)\operatorname{GL}_{6}(2) of all matrices of the form

(6.1) (A𝟎𝟎B𝟎𝟎𝟎1)\displaystyle\begin{pmatrix}A&\mathbf{0}&\mathbf{0}\\ \ast&B&\mathbf{0}\\ \mathbf{0}&\mathbf{0}&1\end{pmatrix}

where ASL3(2)A\in\operatorname{SL}_{3}(2), BSL2(2)B\in\operatorname{SL}_{2}(2), and \ast denotes an arbitrary 2×32\times 3 matrix.

First, write (23)a(2^{3})_{a} for the non-toral subgroup 232^{3} arising from E6E_{6}. This remains non-toral in GG by [22, Remark 8.4], has distribution 2B72{\rm B}_{7} in GG, and we have shown above that it lies in the G2G_{2} factor of a subgroup of type A2G2A_{2}G_{2}, maximal among connected subgroups of E6(K)E_{6}(K). Since the centraliser in GG of the factor G2G_{2} contains a subgroup A2A_{2}, by inspecting [29, Table 8.2] it follows that the connected centraliser of this G2G_{2} factor is simple of type C3C_{3}. Using Lemma 3.5, we deduce that CG((23)a)C_{G}((2^{3})_{a}) has dimension 2121, and therefore CG((23)a)C_{G}((2^{3})_{a})^{\circ} is simple of type C3C_{3}. Inspecting [29, Tables 8.2 and 8.6] also shows that the centre of this subgroup of type C3C_{3} equals Z(G)=zZ(G)=\langle z\rangle since it acts trivially on L(G)L(G). Now the subgroup of GG of type G2C3G_{2}C_{3} is a maximal subgroup of GG, and so each factor is the full centraliser of the other. Hence NG((23)a)NG(CG((23)a))=G2(K)×Sp6(K)N_{G}((2^{3})_{a})\leq N_{G}(C_{G}((2^{3})_{a})^{\circ})=G_{2}(K)\times\operatorname{Sp}_{6}(K). It follows that

NG((23)a)=(23:SL3(2))×Sp6(K)andCG((23)a)=23×Sp6(K).N_{G}((2^{3})_{a})=(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{Sp}_{6}(K)\quad\text{and}\quad C_{G}((2^{3})_{a})=2^{3}\times\operatorname{Sp}_{6}(K).

The above also shows that MCG((23)a)G2(K)×Sp6(K)M\leq C_{G}((2^{3})_{a})\leq G_{2}(K)\times\operatorname{Sp}_{6}(K). Since (23)aG2(2^{3})_{a}\leq G_{2} and Z(CG(M))=Z(SL2(K)3)Sp6(K)Z(C_{G}(M)^{\circ})=Z(\operatorname{SL}_{2}(K)^{3})\leq\operatorname{Sp}_{6}(K), we obtain

M=26=(23)a×Z(SL2(K)3)=(MG2(K))×(MSp6(K)).M=2^{6}=(2^{3})_{a}\times Z(\operatorname{SL}_{2}(K)^{3})=(M\cap G_{2}(K))\times(M\cap\operatorname{Sp}_{6}(K)).

We now use this decomposition to describe the GG-classes of elements of MM and the action of NG(M)N_{G}(M). From [31, Table 10.2], the subgroup G2(K)×Sp6(K)G_{2}(K)\times\operatorname{Sp}_{6}(K) acts on the 5656-dimensional GG-module with two composition factors; one is a tensor product V7V6V_{7}\otimes V_{6} of the natural 77- and 66-dimensional modules for G2(K)G_{2}(K) and Sp6(K)\operatorname{Sp}_{6}(K), denoted in [31] by their highest weights ‘1010’ and ‘100100’. The other is a 1414-dimensional irreducible Sp6(K)\operatorname{Sp}_{6}(K)-module, V14V_{14} (highest weight ‘001001’). Straightforward weight calculations show that the alternating third power of V6V_{6} is isomorphic to V6V14V_{6}\oplus V_{14} as an Sp6(K)\operatorname{Sp}_{6}(K)-module. Hence the eigenvalues of an element on V14V_{14} can be determined directly from those on V6V_{6}. In particular, letting χ7\chi_{7}, χ6\chi_{6}, and χ14\chi_{14} denote the characters of the three respective modules, if x(23)ax\in(2^{3})_{a} and yZ(SL2(K)3)y\in Z(\operatorname{SL}_{2}(K)^{3}), then χmin(xy)=χ7(x)χ6(y)+χ14(y)\chi_{\rm min}(xy)=\chi_{7}(x)\chi_{6}(y)+\chi_{14}(y); see Section 3.3 for the definition of χmin\chi_{\rm min}. For i=1,2,3i=1,2,3, let yiy_{i} be a generator of the centre of the ii-th factor in SL2(K)3\operatorname{SL}_{2}(K)^{3}, and write z=y1y2y3Z(G)z=y_{1}y_{2}y_{3}\in Z(G). Each yiy_{i} is Sp6(K)\operatorname{Sp}_{6}(K)-conjugate to a diagonal matrix diag(1,1,1,1,1,1)\operatorname{diag}(-1,-1,1,1,1,1), hence has trace 22 on V6V_{6} and 6-6 on V14V_{14}. The products yiyjy_{i}y_{j} (ij)(i\neq j) have trace 2-2 on V6V_{6} and 66 on V14V_{14}, and y1y2y3y_{1}y_{2}y_{3} has trace 6-6 on V6V_{6} and 14-14 on V14V_{14}. Therefore if x(23)ax\in(2^{3})_{a} and yZ(SL2(K)3)y\in Z(\operatorname{SL}_{2}(K)^{3}), we find

χmin(xy)={56x=1,y=156x=1,y=y1y2y3(=z)8x=1,y{y1,y2,y3},or x1,y{1,y1y2,y2y3,y1y3}8x1,y{y1,y2,y3,z},or x=1,y{y1y2,y2y3,y1y3}\small\chi_{\rm min}(xy)=\left\{\begin{array}[]{rll}56&\textup{:\ }x=1,\ y=1\\ -56&\textup{:\ }x=1,\ y=y_{1}y_{2}y_{3}(=z)\\ 8&\textup{:\ }x=1,\ y\in\{y_{1},y_{2},y_{3}\},&\textup{or }x\neq 1,\ y\in\{1,y_{1}y_{2},y_{2}y_{3},y_{1}y_{3}\}\\ -8&\textup{:\ }x\neq 1,\ y\in\{y_{1},y_{2},y_{3},z\},&\textup{or }x=1,\ y\in\{y_{1}y_{2},y_{2}y_{3},y_{1}y_{3}\}\end{array}\right.

which allows us to determine the distribution of MM via Table 1 as 2A1B31C312{\rm A}_{1}{\rm B}_{31}{\rm C}_{31}. Now, NG(M)N_{G}(M) acts on SL2(K)3\operatorname{SL}_{2}(K)^{3}, and hence on {y1,y2,y3}\{y_{1},y_{2},y_{3}\}, via its subgroup Sym3\operatorname{Sym}_{3}. The subgroup (23)a×y1y2,y2y3(2^{3})_{a}\times\left<y_{1}y_{2},y_{2}y_{3}\right> is then the unique subgroup of MM containing all 2B2{\rm B}-involutions not lying in the NG(M)N_{G}(M)-orbit {y1,y2,y3}\{y_{1},y_{2},y_{3}\}, and is therefore NG(M)N_{G}(M)-invariant. Thus if (23)a=x1,x2,x3(2^{3})_{a}=\left<x_{1},x_{2},x_{3}\right> then NG(M)N_{G}(M) preserves the direct-product decomposition M=26=x1,x2,x3,y1y2,y2y3×zM=2^{6}=\langle x_{1},x_{2},x_{3},y_{1}y_{2},y_{2}y_{3}\rangle\times\left<z\right>, and taking the elements shown as an ordered vector space basis for MM, we realise NG(M)/CG(M)N_{G}(M)/C_{G}(M) as the set of matrices as in (6.1) above.

Now define (23)b=x1,x2,zx3(2^{3})_{b}=\left<x_{1},x_{2},zx_{3}\right>, and note that CG((23)b)=CG((23)a)C_{G}((2^{3})_{b})=C_{G}((2^{3})_{a}), so (23)b(2^{3})_{b} is non-toral by Lemma 3.5 and has distribution 2B3C42{\rm B}_{3}{\rm C}_{4} by Table 1. A direct calculation with (6.1) shows that NG(M)N_{G}(M) has eleven orbits on subgroups of MM containing a conjugate of (23)a(2^{3})_{a} or (23)b(2^{3})_{b}: in addition to the subgroups MM, (23)a(2^{3})_{a}, and (23)b(2^{3})_{b}, there are subgroups

(24)a\displaystyle(2^{4})_{a} =2A1B7C7=x1,x2,x3,z,\displaystyle=2{\rm A}_{1}{\rm B}_{7}{\rm C}_{7}=\left<x_{1},x_{2},x_{3},z\right>, (24)b\displaystyle(2^{4})_{b} =2B14C1=x1,x2,x3,zy1,\displaystyle=2{\rm B}_{14}{\rm C}_{1}=\left<x_{1},x_{2},x_{3},zy_{1}\right>,
(24)c\displaystyle(2^{4})_{c} =2B8C7=x1,x2,x3,y1,\displaystyle=2{\rm B}_{8}{\rm C}_{7}=\left<x_{1},x_{2},x_{3},y_{1}\right>, (24)d\displaystyle(2^{4})_{d} =2B6C9=x1,x2,zx3,zy1,\displaystyle=2{\rm B}_{6}{\rm C}_{9}=\left<x_{1},x_{2},zx_{3},zy_{1}\right>,
(25)a\displaystyle(2^{5})_{a} =2A1B15C15=x1,x2,x3,y1,z,\displaystyle=2{\rm A}_{1}{\rm B}_{15}{\rm C}_{15}=\left<x_{1},x_{2},x_{3},y_{1},z\right>, (25)b\displaystyle(2^{5})_{b} =2B28C3=x1,x2,x3,zy1,zy2,\displaystyle=2{\rm B}_{28}{\rm C}_{3}=\left<x_{1},x_{2},x_{3},zy_{1},zy_{2}\right>,
(25)c\displaystyle(2^{5})_{c} =2B16C15=x1,x2,x3,y1,y2,\displaystyle=2{\rm B}_{16}{\rm C}_{15}=\left<x_{1},x_{2},x_{3},y_{1},y_{2}\right>, (25)d\displaystyle(2^{5})_{d} =2B12C19=x1,x2,zx3,zy1,zy2.\displaystyle=2{\rm B}_{12}{\rm C}_{19}=\left<x_{1},x_{2},zx_{3},zy_{1},zy_{2}\right>.

Each such subgroup is non-toral, and their distributions (given in Table 5) show that the subgroups are pairwise non-conjugate in GG. There are 1515 further NG(M)N_{G}(M)-orbits on subgroups of MM of rank 33 or more, and each of these has an MM-conjugate contained in the subgroup x1,x2,y1,y2,y3\left<x_{1},x_{2},y_{1},y_{2},y_{3}\right>. We claim that this subgroup, and therefore all of its subgroups, are toral. By construction, x1,x2,x3\left<x_{1},x_{2},x_{3}\right> is contained in a subgroup G2G_{2} and y1,y2,y3\left<y_{1},y_{2},y_{3}\right> is a central subgroup of SL2(K)3\operatorname{SL}_{2}(K)^{3}, which is in turn contained in a simple subgroup of type C3C_{3}, and these subgroups G2G_{2} and C3C_{3} commute. Moreover, x1,x2\left<x_{1},x_{2}\right> is toral in G2(K)G_{2}(K), and y1,y2,y3\left<y_{1},y_{2},y_{3}\right> is toral in SL2(K)3\operatorname{SL}_{2}(K)^{3} by Lemma 3.5. The claim follows.

Centralisers. We now determine centralisers. Each subgroup above is generated by either (23)a(2^{3})_{a} or (23)b(2^{3})_{b} together with some involutions in Sp6(K)\operatorname{Sp}_{6}(K). The Sp6(K)\operatorname{Sp}_{6}(K)-centraliser of a non-central involution is SL2(K)×Sp4(K)\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K), and it is then straightforward to see that the Sp6(K)\operatorname{Sp}_{6}(K)-centraliser of an elementary abelian 22-subgroup of Sp6(K)\operatorname{Sp}_{6}(K) is either Sp6(K)\operatorname{Sp}_{6}(K) itself, or SL2(K)×Sp4(K)\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K), or SL2(K)3\operatorname{SL}_{2}(K)^{3}. This determines the centraliser of every non-toral subgroup of MM.

Normalisers. It remains to determine the normaliser quotient NG(E)/CG(E)N_{G}(E)/C_{G}(E) for each subgroup EE. Firstly, the non-toral subgroups of E6E_{6} remain non-toral in GG under the inclusion 3.E6(K)G3.E_{6}(K)\to G as they each contain (23)a(2^{3})_{a}. These three subgroups are each contained in a subgroup F4(K)F_{4}(K) by construction, and then [41, Propositions 5.4 and 5.5] show that every possible class-preserving automorphism of such a subgroup is already induced by conjugation by an element of F4(K)F_{4}(K), hence the subgroups (23)a(2^{3})_{a}, (24)b(2^{4})_{b}, and (25)b(2^{5})_{b} with distributions 2B72{\rm B}_{7}, 2B14C12{\rm B}_{14}{\rm C}_{1} and 2B28C32{\rm B}_{28}{\rm C}_{3} have the same normaliser quotient as in E6(K)E_{6}(K), and in F4(K)F_{4}(K). For E=(23)bE=(2^{3})_{b}, any automorphism induced by conjugation in GG must preserve the subgroup x1,x2\left<x_{1},x_{2}\right> as this is generated by all 2B2{\rm B}-involutions in EE. The group SL3(2)\operatorname{SL}_{3}(2) of automorphisms of (23)a(2^{3})_{a} centralises zz, and the stabiliser of x1,x2\left<x_{1},x_{2}\right> in SL3(2)\operatorname{SL}_{3}(2) induces all such automorphisms on (23)b(2^{3})_{b}. It follows that NG(E)/CG(E)=22.SL2(2)N_{G}(E)/C_{G}(E)=2^{2}.\operatorname{SL}_{2}(2) is the stabiliser of a 22-dimensional subspace.

A direct calculation shows that if E=(24)aE=(2^{4})_{a} or E=(24)cE=(2^{4})_{c}, then EE contains a unique 2B2{\rm B}-pure subgroup of order 88, namely (23)a(2^{3})_{a}, and so NG(E)NG((23)a)=((23:SL3(2))×Sp6(K)N_{G}(E)\leq N_{G}((2^{3})_{a})=((2^{3}\mathpunct{:}\operatorname{SL}_{3}(2))\times\operatorname{Sp}_{6}(K). Since y1y_{1}, zz, and y1zy_{1}z are involutions in Sp6(K)\operatorname{Sp}_{6}(K) lying in distinct GG-conjugacy classes, and since Sp6(K)\operatorname{Sp}_{6}(K) is centralised by the action of SL3(2)\operatorname{SL}_{3}(2), it follows that NG((24)a)/CG((24)a)=NG((24)c)/CG((24)c)=SL3(2)N_{G}((2^{4})_{a})/C_{G}((2^{4})_{a})=N_{G}((2^{4})_{c})/C_{G}((2^{4})_{c})=\operatorname{SL}_{3}(2). The group E=(24)dE=(2^{4})_{d} contains a unique subgroup E0E_{0} with distribution 2B6C12{\rm B}_{6}{\rm C}_{1}, and this in turn contains a unique involution in class 2C2{\rm C}; thinking of NG(E)/CG(E)N_{G}(E)/C_{G}(E) as a subgroup of GL4(2)\operatorname{GL}_{4}(2), it is contained in the set of matrices of the form

(1𝟎𝟎A𝟎1)\begin{pmatrix}1&\mathbf{0}&\mathbf{0}\\ \ast&A&\mathbf{0}\\ \ast&\ast&1\end{pmatrix}

with AGL2(2)A\in\operatorname{GL}_{2}(2). The NG(M)N_{G}(M)-stabiliser of (24)d(2^{4})_{d} induces all such automorphisms, giving the stated normaliser structure NG(E)/CG(E)=21+4.Sym3N_{G}(E)/C_{G}(E)=2^{1+4}.\operatorname{Sym}_{3}. Similarly, E=(25)aE=(2^{5})_{a} contains a unique subgroup E0E_{0} with distribution 2B14C12{\rm B}_{14}{\rm C}_{1} and NG(E)N_{G}(E) preserves the direct-sum decomposition E=E0×zE=E_{0}\times\langle z\rangle. Moreover, E0E_{0} contains a unique involution in class 2C2{\rm C}. Hence NG(E)/CG(E)N_{G}(E)/C_{G}(E) can be identified with a set of matrices of the form

(1𝟎𝟎A𝟎𝟎𝟎1)\begin{pmatrix}1&\mathbf{0}&\mathbf{0}\\ \ast&A&\mathbf{0}\\ \mathbf{0}&\mathbf{0}&1\end{pmatrix}

with AGL3(2)A\in\operatorname{GL}_{3}(2). Again, NG(M)N_{G}(M) induces all such automorphisms, hence we obtain NG(E)/CG(E)=23:SL3(2)N_{G}(E)/C_{G}(E)=2^{3}:\operatorname{SL}_{3}(2). If E=(25)cE=(2^{5})_{c}, then EE contains a unique subgroup E0E_{0} with distribution 2B14C12{\rm B}_{14}{\rm C}_{1}, and E0E_{0} is a conjugate of (24)b(2^{4})_{b}. Thus, NG(E)N_{G}(E) is contained in NG(E0)=(23×SL2(K)×Sp4(K)).(23:SL3(2))N_{G}(E_{0})=(2^{3}\times\operatorname{SL}_{2}(K)\times\operatorname{Sp}_{4}(K)).(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)). The subgroup SL2(K)\operatorname{SL}_{2}(K) centralises MM and thus EE, while the subgroup Sp4(K)\operatorname{Sp}_{4}(K) contains an element swapping y1y_{1} and y2y_{2} (taking y1y2y_{1}y_{2} to be the central element of Sp4(K)\operatorname{Sp}_{4}(K) without loss of generality), and acting trivially on the subgroup x1,x2,x3\left<x_{1},x_{2},x_{3}\right> of EE. Hence NG(E)/CG(E)2×(23:SL3(2))N_{G}(E)/C_{G}(E)\leq 2\times(2^{3}\mathpunct{:}\operatorname{SL}_{3}(2)). We again find that NG(M)N_{G}(M) induces all such automorphisms on EE, so NG(E)/CG(E)=2×(23:SL3(2))N_{G}(E)/C_{G}(E)=2\times(2^{3}:\operatorname{SL}_{3}(2)). Finally, let E=(25)dE=(2^{5})_{d}. This contains a unique subgroup E0E_{0} with distribution 2B12C32{\rm B}_{12}{\rm C}_{3}, and E0E_{0} in turn contains a unique subgroup with distribution 2C32{\rm C}_{3}. Thus NG(E)/CG(E)N_{G}(E)/C_{G}(E) is contained in the set of all matrices of the form

(1𝟎𝟎A𝟎B)\begin{pmatrix}1&\mathbf{0}&\mathbf{0}\\ \ast&A&\mathbf{0}\\ \ast&\ast&B\end{pmatrix}

with A,BGL2(2)A,B\in\operatorname{GL}_{2}(2). Once again, NG(M)N_{G}(M) induces all such automorphisms on EE, so NG(E)/CG(E)N_{G}(E)/C_{G}(E) is determined.

6.7. Proof of Proposition 6.3 for G=E7,ad(K)G=E_{7,{{\text{\rm ad}}}}(K)

Let G=E7,ad(K)G=E_{7,{{\text{\rm ad}}}}(K) and p=2p=2. The three classes of involutions in GG are denoted by 2BC2{\rm BC}, 4A4{\rm A}, and 4H4{\rm H}, corresponding to the classes in the simply connected cover of GG which map onto them (see Section 3.3). In [41], Yu has identified 78 classes of elementary abelian 22-subgroups of GG and determined their normaliser quotients. However, it remains to determine their centraliser structure and whether or not these subgroups are toral. In the course of determining this information, we have found some typographic errors in the ancillary data of [41], particularly in [41, Remark 7.27], although we agree with the eventual classification itself. For this reason, we now carry out a number of our own calculations, verifying much of the information in [41].

The toral elementary abelian 22-subgroups of GG can be determined with our algorithm in Section 5.1. We find that there are 3232 conjugacy classes of such toral subgroups. It follows from [22] that GG has two maximal non-toral subgroups up to conjugacy, of orders 272^{7} and 282^{8}, respectively. Between them, these contain representatives of each class of non-toral subgroups; since the subgroup of order 282^{8} is obtained by adjoining a Chevalley involution to a maximal toral subgroup of order 272^{7}, it also contains a representative of every class of toral subgroups.

By [22, Table 1], the maximal non-toral subgroups 272^{7} and 282^{8} are each self-centralising, and have normaliser quotients as follows

NG(28)/28\displaystyle N_{G}(2^{8})/2^{8} =27:SO7(2)and\displaystyle=2^{7}:\operatorname{SO}_{7}(2)\quad\text{and}
NG(27)/27\displaystyle N_{G}(2^{7})/2^{7} =(222×223):(Sym3×Sym3×SL3(2)).\displaystyle=(2^{2\cdot 2}\times 2^{2\cdot 3})\mathpunct{:}(\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}\times\operatorname{SL}_{3}(2)).

Because NG(27)N_{G}(2^{7}) and NG(28)N_{G}(2^{8}) are finite, and their actions on 272^{7} and 282^{8} are known (cf. [41, Proposition 7.27] and Appendix A.2), we can explicitly construct these groups as matrix groups of degree 77 and 88, respectively. In particular, we can calculate the orbits of these groups on the subgroups of 272^{7} and 282^{8}, using Magma [13]. Our computation also returns the complete subgroup lattice for these groups. Appendix A.3 comments on our construction. Recall that every non-toral subgroup of GG appears as a subgroup of at least one of the maximal 272^{7} and 282^{8}. The (known) distributions of 272^{7} and 282^{8} allow us to identify the distributions of the subgroups in each orbit. From this, together with the information on toral subgroups already calculated, we can determine for most subgroups occurring whether the subgroup is toral or non-toral. A few cases require further arguments, and for these we defer to information from [41]. In the end, we are able to identify 4646 conjugacy classes of non-toral elementary abelian 22-subgroups of GG; these are listed in Table 6. We label these groups according to the classification in [41], see Appendix A.1 for a description of this classification. Our investigations yield the following corollary.

Corollary 6.5.

The complete Hasse diagram of non-toral 22-subgroups in GG is given in Figure 1.

The structure of the normaliser quotients of the groups in Table 6 has been determined in [41, Proposition 7.26], see also Appendix A.2 for more details. In the remainder of this section, we discuss the centralisers of the non-toral subgroups; for this the inclusions implied in the Hasse diagram (Figure 1) will be useful. In most cases, the centraliser of EE with |E|>22|E|>2^{2} is determined in CG(U)C_{G}(U) where E=U,uE=\langle U,u\rangle for some non-toral UU; the column labelled “UU” in Table 6 lists this subgroup, see Case (2) in the proof of Proposition 6.6.

Proposition 6.6.

If EE is as given in Table 6, then CG(E)C_{G}(E) is as given in that table.

Proof.

We consider the following sets of groups as defined in Table 6:

𝒳0\displaystyle\mathcal{X}_{0} ={(22)a,(22)b,(22)c,(23)e,(23)g},\displaystyle=\{(2^{2})_{a},(2^{2})_{b},(2^{2})_{c},(2^{3})_{e},(2^{3})_{g}\},
𝒳1\displaystyle\mathcal{X}_{1} ={(24)j,(25)k,(25)f,(25)h,(26)g,(26)c,(26)b},\displaystyle=\{(2^{4})_{j},(2^{5})_{k},(2^{5})_{f},(2^{5})_{h},(2^{6})_{g},(2^{6})_{c},(2^{6})_{b}\},
𝒳2\displaystyle\mathcal{X}_{2} ={(24)i,(25)i,(25)j,(26)f},\displaystyle=\{(2^{4})_{i},(2^{5})_{i},(2^{5})_{j},(2^{6})_{f}\},

and make a case distinction.

  • (Case 1)

    Suppose E𝒳0E\in\mathcal{X}_{0}. The centraliser of each Klein four-subgroup of a compact simple real Lie group of type E7E_{7} is given in [24, Table 6], and in our three cases (22)a,(22)b,(22)c(2^{2})_{a},(2^{2})_{b},(2^{2})_{c}, this is the direct product of the non-toral subgroup in question with a maximal connected subgroup (in the real topology) of the centraliser in the complex algebraic group; cf. [21, Table 4.3.3]. (Note that [24, Table 6] lists the centraliser Aut(𝔢7)Γ\operatorname{Aut}(\mathfrak{e}_{7})^{\Gamma} of each Klein-four subgroup Γ\Gamma of Aut(𝔢7)\operatorname{Aut}(\mathfrak{e}_{7}), and the latter is a maximal compact subgroup of GG since GG is adjoint.) The centraliser structure for the subgroups of rank 22 in Table 6 follows.

    To consider (23)e(2^{3})_{e} and (23)g(2^{3})_{g}, we need some preliminary results. Let H=E7,scH=E_{7,{\text{\rm sc}}}, so that G=H/ZG=H/Z where Z=Z(H)=zZ=Z(H)=\langle z\rangle. By [21, Tables 4.3.1–4.3.3] there is an involution tHt\in H such that

    CH(t)=Spin12(K)2SL2(K),C_{H}(t)=\operatorname{Spin}_{12}(K)\circ_{2}\operatorname{SL}_{2}(K),

    where the central product is over 2=2s:2Spin12(K)×SL2(K)2=\langle 2_{s}{:}2\rangle\leq\operatorname{Spin}_{12}(K)\times\operatorname{SL}_{2}(K). Note that ZZ(CH(t))Z\leq Z(C_{H}(t)), and Z(CH(t))=2c:1,2s:1=Z(Spin12(K))Z(C_{H}(t))=\langle 2_{c}{:}1,2_{s}{:}1\rangle=Z(\operatorname{Spin}_{12}(K)) where 2s:1=1:22_{s}{:}1=1{:}2 generates Z(SL2(K))Z(\operatorname{SL}_{2}(K)). It follows also from [21, Tables 4.3.1–4.3.3] that tZGtZ\in G has centraliser CG(tZ)=Spin12(K)22SL2(K)C_{G}(tZ)=\operatorname{Spin}_{12}(K)\circ_{2^{2}}\operatorname{SL}_{2}(K), where the central product is over 22=2s:1,2c:22^{2}=\langle 2_{s}{:}1,2_{c}{:}2\rangle. This shows that CG(tZ)=CH(t)/ZC_{G}(tZ)=C_{H}(t)/Z. Since Z(CG(tZ))=2Z(C_{G}(tZ))=2 is generated by 2c:12_{c}{:}1, it follows that Z=2s:1Z=\langle 2_{s}{:}1\rangle is contained in Spin12(K)2SL2(K)\operatorname{Spin}_{12}(K)\circ_{2}\operatorname{SL}_{2}(K), so z=2s:1=1:2z=2_{s}{:}1=1{:}2 lies in Z(SL2(K))Z(\operatorname{SL}_{2}(K)). A direct computation shows that there is a toral X=22HX=2^{2}\leq H with tXt\in X such that CH(X)=A5T2C_{H}(X)^{\circ}=A_{5}T_{2} and CH(X)=CH(X).w=CH(X).2C_{H}(X)=C_{H}(X)^{\circ}.w=C_{H}(X)^{\circ}.2, and OutH(X)=Sym3\operatorname{Out}_{H}(X)=\operatorname{Sym}_{3}. Let X=t,yX=\langle t,y\rangle for some involution y=y1:y2CH(t)y=y_{1}{:}y_{2}\in C_{H}(t). Since CCH(t)(y)=A5T2C_{C_{H}(t)}(y)^{\circ}=A_{5}T_{2}, it follows that CSL2(K)(y2)=T1C_{\operatorname{SL}_{2}(K)}(y_{2})^{\circ}=T_{1} and CSpin12(K)(y1)=A5T1C_{\operatorname{Spin}_{12}(K)}(y_{1})^{\circ}=A_{5}T_{1}.

    By [21, Tables 4.3.1–4.3.3], there is a projective involution u1Spin12(K)u_{1}\in\operatorname{Spin}_{12}(K) such that CSpin12(K)(u1)=SL6(K)3T1C_{\operatorname{Spin}_{12}(K)}(u_{1})=\operatorname{SL}_{6}(K)\circ_{3^{*}}T_{1}, where 3=gcd(3,1)3^{*}=\gcd(3,\ell-1) with \ell being the characteristic of KK. Choose a subgroup u2,v2SL2(K)\langle u_{2},v_{2}\rangle\leq\operatorname{SL}_{2}(K) isomorphic to Q8Q_{8} with u22=v22=zu_{2}^{2}=v_{2}^{2}=z. By [21, Tables 4.3.1–4.3.3], we may suppose y2=u2y_{2}=u_{2}, and so y12=y22=zy_{1}^{2}=y_{2}^{2}=z; this shows that y1Spin12(K)y_{1}\in\operatorname{Spin}_{12}(K) is a projective involution as well. By [21, Tables 4.3.1-4.3.3], we may suppose y1=u1y_{1}=u_{1}, so

    CH(X)=(T23SL6(K)).w.C_{H}(X)=(T_{2}\circ_{3^{*}}\operatorname{SL}_{6}(K)).w.

    Now write w=w1:w2CH(t)w=w_{1}{:}w_{2}\in C_{H}(t) with w1Spin12(K)w_{1}\in\operatorname{Spin}_{12}(K) and w2SL2(K)w_{2}\in\operatorname{SL}_{2}(K). It follows from [21, Table 4.3.1] that w2w_{2} acts via inversion on T1T_{1}; note that w2w_{2} normalizes CSL2(K)(y2)=T1C_{\operatorname{SL}_{2}(K)}(y_{2})=T_{1}. This implies that w2w_{2} centralises CSL2(K)/Z(y2Z)C_{\operatorname{SL}_{2}(K)/Z}(y_{2}Z), so w1w_{1} centralises CSpin12(K)/Z(y1Z)C_{\operatorname{Spin}_{12}(K)/Z}(y_{1}Z). By [21, Table 4.3.1], the element w1w_{1} induces γ:i\gamma{:}i on SL6(K)3T1\operatorname{SL}_{6}(K)\circ_{3^{*}}T_{1}; here γ\gamma and ii denote a graph automorphism and inversion, respectively. It follows that ww acts via inversion on T2T_{2} and induces a graph automorphism on SL6(K)\operatorname{SL}_{6}(K). Note that OutH(X)=Sym3\operatorname{Out}_{H}(X)=\operatorname{Sym}_{3} acts on both Z(CH(X))=2×T2Z(C_{H}(X)^{\circ})=2\times T_{2} and Z(SL6(K))=2×3Z(\operatorname{SL}_{6}(K))=2\times 3^{*}. Moreover, we have X2×(T2)(2)X\leq 2\times(T_{2})_{(2)}, and it follows that Sym3\operatorname{Sym}_{3} centralises Z(SL6(K))2=2Z(\operatorname{SL}_{6}(K))_{2}=2. If ZZ(SL6(K))2Z\neq Z(\operatorname{SL}_{6}(K))_{2}, then Sym3\operatorname{Sym}_{3} centralises at least two distinct involutions in 2×(T2)(2)2\times(T_{2})_{(2)}, which is impossible; this proves that ZZ(SL6(K))Z\leq Z(\operatorname{SL}_{6}(K)). Let Y=XZ=23Y=XZ=2^{3}, so that CH(Y)=CH(X)C_{H}(Y)=C_{H}(X). Note that Y/ZY/Z is toral in GG and CG(Y/Z)CH(X)/ZC_{G}(Y/Z)\geq C_{H}(X)/Z. A direct computation shows that Y/Z=22=2BC3Y/Z=2^{2}=2{\rm B}{\rm C}_{3} and it yields that

    CG(Y/Z)=(T23(SL6(K)/Z)).g,C_{G}(Y/Z)=(T_{2}\circ_{3^{*}}(\operatorname{SL}_{6}(K)/Z)).g,

    where g=wZg=wZ acts via inversion on T2T_{2} and induces a graph automorphism on SL6(K)\operatorname{SL}_{6}(K).

    Now consider E=Y/Z,x=23E=\langle Y/Z,x\rangle=2^{3} for some xCG(Y/Z)CG(Y/Z)x\in C_{G}(Y/Z)\setminus C_{G}(Y/Z)^{\circ}; in particular, CT2(x)=22C_{T_{2}}(x)=2^{2}, and xx induces a graph automorphism on SL6(K)\operatorname{SL}_{6}(K). By [21, Tables 4.3.1–4.3.3], there are two graph automorphisms, γ1\gamma_{1} and γ2\gamma_{2}, such that CSL6(K)(γ1)=Sp6(K)C_{\operatorname{SL}_{6}(K)}(\gamma_{1})=\operatorname{Sp}_{6}(K) and CSL6(K)(γ2)=SO6(K)C_{\operatorname{SL}_{6}(K)}(\gamma_{2})=\operatorname{SO}_{6}(K), and CPSL6(K)(γ1)=PSp6(K)C_{{\rm PSL}_{6}(K)}(\gamma_{1})={\rm PSp}_{6}(K) and CPSL6(K)(γ2)=PSO6(K).γC_{{\rm PSL}_{6}(K)}(\gamma_{2})={\rm PSO}_{6}(K).\gamma. Note that each group Y/Z,γi\langle Y/Z,\gamma_{i}\rangle is non-toral. Comparing dimensions, we can therefore suppose that

    (23)g=Y/Z,γ1and(23)e=Y/Z,γ2;(2^{3})_{g}=\langle Y/Z,\gamma_{1}\rangle\quad\text{and}\quad(2^{3})_{e}=\langle Y/Z,\gamma_{2}\rangle;

    in particular, we can assume that Y/ZY/Z is a subgroup of (23)g(2^{3})_{g} and (23)e(2^{3})_{e}. If 3=13^{*}=1, then it follows from above that CG(Y/Z)=(T2×PSL6(K)).xC_{G}(Y/Z)=(T_{2}\times{\rm PSL}_{6}(K)).x, so CG((23)g)=23×PSp6(K)C_{G}((2^{3})_{g})=2^{3}\times{\rm PSp}_{6}(K) and CG((23)e)=23×PSO6(K).γC_{G}((2^{3})_{e})=2^{3}\times{\rm PSO}_{6}(K).\gamma, as claimed. If 3=33^{*}=3, then Z(SL6(K))=U=6Z(\operatorname{SL}_{6}(K))=U=6 and each CU(γi)=ZC_{U}(\gamma_{i})=Z. Write V=U/ZV=U/Z and note that

    CSL6(K)(γ1)/UCSL6(K)/Z(γ1)/VCPSL6(K)(γ1).C_{\operatorname{SL}_{6}(K)}(\gamma_{1})/U\leq C_{\operatorname{SL}_{6}(K)/Z}(\gamma_{1})/V\leq C_{{\rm PSL}_{6}(K)}(\gamma_{1}).

    This yields CSL6(K)(γ1)/U=PSp6(K)=CPSL6(K)(γ1)C_{\operatorname{SL}_{6}(K)}(\gamma_{1})/U={\rm PSp}_{6}(K)=C_{{\rm PSL}_{6}(K)}(\gamma_{1}), and it then follows that CSL6(K)/Z(γ1)=Sp6(K)/Z=PSp6(K)C_{\operatorname{SL}_{6}(K)/Z}(\gamma_{1})=\operatorname{Sp}_{6}(K)/Z={\rm PSp}_{6}(K) and CG((23)g)=23×PSp6(K)C_{G}((2^{3})_{g})=2^{3}\times{\rm PSp}_{6}(K), as claimed. Similarly, we deduce that

    PSO6(K)CSL6(K)/Z(γ2)PSO6(K).γ.{\rm PSO}_{6}(K)\leq C_{\operatorname{SL}_{6}(K)/Z}(\gamma_{2})\leq{\rm PSO}_{6}(K).\gamma.

    Let hSL6(K)/Zh\in\operatorname{SL}_{6}(K)/Z such that hV=γCPSL6(K)(γ2)=PSO6(K).γhV=\gamma\in C_{{\rm PSL}_{6}(K)}(\gamma_{2})={\rm PSO}_{6}(K).\gamma. Since γ2\gamma^{2} acts trivially on PSO6(K){\rm PSO}_{6}(K), it follows that h2Z(SL6(K)/Z)=Vh^{2}\in Z(\operatorname{SL}_{6}(K)/Z)=V, and so hh has order 22 or 66. Replacing hh by h3h^{3}, if necessary, we may suppose that |h|=2|h|=2. Now (hV)γ2=hV(hV)^{\gamma_{2}}=hV, and so hγ2hVh^{\gamma_{2}}\in hV. Since |hγ2|=2|h^{\gamma_{2}}|=2, it follows that hγ2=hh^{\gamma_{2}}=h and therefore CSL6(K)/Z(γ2)=PSO6(K).γC_{\operatorname{SL}_{6}(K)/Z}(\gamma_{2})={\rm PSO}_{6}(K).\gamma. This shows that CG((23)e)=23×PSO6(K).γC_{G}((2^{3})_{e})=2^{3}\times{\rm PSO}_{6}(K).\gamma, as claimed.

  • (Case 2)

    Suppose EG𝒳0E\not\in_{G}\mathcal{X}_{0}. It follows from Figure 1 that E=U,uE=\langle U,u\rangle for some non-toral elementary abelian subgroup UU containing some subgroup V𝒳0V\in\mathcal{X}_{0}, and an involution uu in CG(U)UC_{G}(U)\setminus U. In particular,

    CG(E)CG(U)CG(V)=2i×N.cC_{G}(E)\leq C_{G}(U)\leq C_{G}(V)=2^{i}\times N.c

    for some i{2,3}i\in\{2,3\} and N{PSO6(K),PSp6(K),F4(K),PSp8(K),PΩ8(K)}N\in\{{\rm PSO}_{6}(K),{\rm PSp}_{6}(K),F_{4}(K),{\rm PSp}_{8}(K),{\rm P}\Omega_{8}(K)\} and c{1,γ}c\in\{1,\gamma\}, see Table 6. Thus, CG(U)C_{G}(U)^{\circ} is a reductive group and uu acts on CG(U)C_{G}(U)^{\circ}. The centralisers of involutions of CG(U)C_{G}(U)^{\circ} can be determined by [21, Tables 4.3.1–4.3.3]; note that CG(E)=CCG(U)(u)C_{G}(E)=C_{C_{G}(U)}(u) and dimCG(E)=dimCCG(U)(u)\dim C_{G}(E)=\dim C_{C_{G}(U)^{\circ}}(u). We use this information to determine CG(E)C_{G}(E); the subgroups UU we use are listed in Table 6.

  • (Case 2a)

    First suppose EG𝒳1𝒳2E\not\in_{G}\mathcal{X}_{1}\cup\mathcal{X}_{2}. By the choice of UU, it follows from [21, Tables 4.3.1–4.3.3] that uu is uniquely determined, up to conjugacy in CG(U)C_{G}(U), by the dimension dimCCG(U)(u)\dim C_{C_{G}(U)^{\circ}}(u), and so CG(E)=CCG(U)(u)C_{G}(E)=C_{C_{G}(U)}(u) can be determined by [21, Tables 4.3.1–4.3.3]. For example, if E=(23)fE=(2^{3})_{f}, then CG(E)C_{G}(E) has dimension 1212. By Figure 1, we have E=U,uE=\langle U,u\rangle with U=(22)cU=(2^{2})_{c} and CG(U)=22×PΩ8(K)C_{G}(U)=2^{2}\times{\rm P}\Omega_{8}(K). It follows from [21, Tables 4.3.1–4.3.3] that PΩ8(K)\text{P}\Omega_{8}(K) contains a unique involution uu such that dimCPΩ8(K)(u)=12\dim C_{P\Omega_{8}(K)}(u)=12. In fact, CPΩ8(K)(u)=(SO4(K)2SO4(K))).γ:γ,C_{{\rm P}\Omega_{8}(K)}(u)=(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K))).\langle\gamma{:}\gamma,\leftrightarrow\rangle, thus

    CG(E)=22×(SO4(K)2SO4(K))).γ:γ,=22×(SO4(K)2SO4(K))).22.C_{G}(E)=2^{2}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K))).\langle\gamma{:}\gamma,\leftrightarrow\rangle=2^{2}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K))).2^{2}.

    The centraliser structure of the other groups EG𝒳1𝒳2E\not\in_{G}\mathcal{X}_{1}\cup\mathcal{X}_{2} can be obtained similarly; we give a few details for (24)x(2^{4})_{x} with x{a,c,e,h}x\in\{a,c,e,h\}:

    • \bullet

      We have (24)c=(23)b,u(2^{4})_{c}=\langle(2^{3})_{b},u\rangle with uSpin9(K)u\in\operatorname{Spin}_{9}(K); since Spin9(K)\operatorname{Spin}_{9}(K) is simply connected, the centraliser CSpin9(K)(u)=Spin8(K)C_{\operatorname{Spin}_{9}(K)}(u)=\operatorname{Spin}_{8}(K) is connected, hence CG((24)c)=22×Spin8(K)C_{G}((2^{4})_{c})=2^{2}\times\operatorname{Spin}_{8}(K).

    • \bullet

      We have (24)e=(23)d,u(2^{4})_{e}=\langle(2^{3})_{d},u\rangle and CG((23)d)=22×(Sp4(K)2Sp4(K)).2C_{G}((2^{3})_{d})=2^{2}\times(\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K)).2. Consider the element v=I2×(I2)Sp4(K)v=I_{2}\times(-I_{2})\in\operatorname{Sp}_{4}(K) and let ww be a permutation matrix corresponding to (1,3)(2,4)(1,3)(2,4), so that [v,w]=I4Z(Sp4(K))[v,w]=-I_{4}\in Z(\operatorname{Sp}_{4}(K)), CSp4(K)(v)=(SL2(K))2C_{\operatorname{Sp}_{4}(K)}(v)=(\operatorname{SL}_{2}(K))^{2}, and ww swaps the two factors of CSp4(K)(v)C_{\operatorname{Sp}_{4}(K)}(v). If u=vvSp4(K)2Sp4(K)u=vv\in\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K), then the outside 2 of (Sp4(K)2Sp4(K)).2(\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K)).2 centralises uu, and so does and w:wSp4(K)2Sp4(K)w{:}w\in\operatorname{Sp}_{4}(K)\circ_{2}\operatorname{Sp}_{4}(K); hence CG((24)e)=22×((SL2(K))22(SL2(K))2).22C_{G}((2^{4})_{e})=2^{2}\times((\operatorname{SL}_{2}(K))^{2}\circ_{2}(\operatorname{SL}_{2}(K))^{2}).2^{2}.

    • \bullet

      We have (24)h=(23)c,u(2^{4})_{h}=\langle(2^{3})_{c},u\rangle with CG((23)c)=22×(GL4(K)/Z).γC_{G}((2^{3})_{c})=2^{2}\times(\operatorname{GL}_{4}(K)/Z).\gamma. Let v=diag(s,s,s1,s1)v=\operatorname{diag}(s,s,s^{-1},s^{-1}) be in GL4(K)\operatorname{GL}_{4}(K) with |s|=4|s|=4 and let wGL4(K)w\in\operatorname{GL}_{4}(K) be the permutation matrix corresponding to (1,3)(2,4)(1,3)(2,4). Then CGL4(K)(v)=GL2(K)2C_{\operatorname{GL}_{4}(K)}(v)=\operatorname{GL}_{2}(K)^{2} and [v,w]=I4Z(GL4(K))[v,w]=-I_{4}\in Z(\operatorname{GL}_{4}(K)). Note that the graph automorphism γ\gamma in (GL4(K)/Z).γ(\operatorname{GL}_{4}(K)/Z).\gamma also gives [v,γ]=I4[v,\gamma]=-I_{4}; if u=vZu=vZ and y=wZy=wZ, then CG((24)h)=22×((GL2(K))2/Z).y.γC_{G}((2^{4})_{h})=2^{2}\times((\operatorname{GL}_{2}(K))^{2}/Z).y.\gamma.

    • \bullet

      We have (24)a=(23)a,u(2^{4})_{a}=\langle(2^{3})_{a},u\rangle with uSL2(K)2Sp6(K)u\in\operatorname{SL}_{2}(K)\circ_{2}\operatorname{Sp}_{6}(K). Write u=u1:u2u=u_{1}{:}u_{2} with u1SL2(K)u_{1}\in\operatorname{SL}_{2}(K) and u2Sp6(K)u_{2}\in\operatorname{Sp}_{6}(K), and note that CSL2(K)(u1)=T1C_{\operatorname{SL}_{2}(K)}(u_{1})=T_{1}, so that |u1|=4|u_{1}|=4 with u12=I2u_{1}^{2}=-I_{2}. Similarly, CSp6(K)(u2)=GL3(K)C_{\operatorname{Sp}_{6}(K)}(u_{2})=\operatorname{GL}_{3}(K) and u22=I6Z(Sp6(K))u_{2}^{2}=-I_{6}\in Z(\operatorname{Sp}_{6}(K)). Let v1SL2(K)v_{1}\in\operatorname{SL}_{2}(K) and v2Sp6(K)v_{2}\in\operatorname{Sp}_{6}(K) such that [u1,v1]=I2[u_{1},v_{1}]=-I_{2} and [u2,v2]=I6[u_{2},v_{2}]=-I_{6}, so that v1v_{1} inverts CSL2(K)(u1)=T1C_{\operatorname{SL}_{2}(K)}(u_{1})=T_{1} and v2v_{2} induces inverse-transpose on CSp6(K)(u2)=GL3(K)C_{\operatorname{Sp}_{6}(K)}(u_{2})=\operatorname{GL}_{3}(K). Thus, v2v_{2} inverts T1=Z(GL3(K))T_{1}=Z(\operatorname{GL}_{3}(K)) and induces a graph automorphism on SL3(K)GL3(K)\operatorname{SL}_{3}(K)\leq\operatorname{GL}_{3}(K). Now u=u1:u2SL2(K)Sp6(K)u=u_{1}{:}u_{2}\in\operatorname{SL}_{2}(K)\circ\operatorname{Sp}_{6}(K) is an involution with CSL2(K)Sp6(K)(u)=T23SL3(K)C_{\operatorname{SL}_{2}(K)\circ\operatorname{Sp}_{6}(K)}(u)=T_{2}\circ_{3^{\ast}}\operatorname{SL}_{3}(K). The element v1:v2v_{1}{:}v_{2} centralises uu, inverts T2=T12T1T_{2}=T_{1}\circ_{2}T_{1}, and induces γ\gamma on SL3(K)\operatorname{SL}_{3}(K).

    Note that (25)b=(24)a,u(2^{5})_{b}=\langle(2^{4})_{a},u\rangle with CG((24)a)=22×(T23SL3(K)).(i:γ)C_{G}((2^{4})_{a})=2^{2}\times(T_{2}\circ_{3}\operatorname{SL}_{3}(K)).(i{:}\gamma); choose u=i:γu=i{:}\gamma with CT2(i)=22C_{T_{2}}(i)=2^{2} and CSL3(K)(γ)=SO3(K)×γ=PGL2(K)×2C_{\operatorname{SL}_{3}(K)}(\gamma)=\text{SO}_{3}(K)\times\langle\gamma\rangle={\rm PGL}_{2}(K)\times 2. For (25)a(2^{5})_{a} note that i:γi{:}\gamma acts on T32SL2(K)T_{3}\circ_{2}\operatorname{SL}_{2}(K) but the graph automorphism γ\gamma acts like an inner automorphism of SL2(K)\operatorname{SL}_{2}(K); thus we can replace i:γi{:}\gamma by i:1i{:}1.

  • (Case 2b)

    Suppose E𝒳1E\in\mathcal{X}_{1}. The methods described in Section 5.1 assist us with determining CG(E)C_{G}(E). For example, if E=(24)jE=(2^{4})_{j}, then EE is the only subgroup of size 242^{4} with dimCG(E)=4\dim C_{G}(E)=4. We take U=(23)f>(22)cU=(2^{3})_{f}>(2^{2})_{c}, so CG((23)f)=22×(SO4(K)2SO4(K))).22CG((22)c)=22×PΩ8(K)C_{G}((2^{3})_{f})=2^{2}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K))).2^{2}\leq C_{G}((2^{2})_{c})=2^{2}\times{\rm P}\Omega_{8}(K), and a direct computation shows that PΩ8(K){\rm P}\Omega_{8}(K) has an elementary abelian subgroup X=22X=2^{2} such that CPΩ8(K)(X)=T4.2+1+4C_{{\rm P}\Omega_{8}(K)}(X)=T_{4}.2_{+}^{1+4}. Thus, CG(U,X)=22×T4.2+1+4C_{G}(\langle U,X\rangle)=2^{2}\times T_{4}.2_{+}^{1+4} and E=U,XE=\langle U,X\rangle by the uniqueness of dimCG(E)\dim C_{G}(E). Note that the action of 2+1+42_{+}^{1+4} is also explicitly determined. The centraliser structure of the other E𝒳1E\in\mathcal{X}_{1} can be obtained similarly. For example, the group (25)h=(24)g,u(2^{5})_{h}=\langle(2^{4})_{g},u\rangle can be defined via a subgroup Q8=v,wSL2(K)Q_{8}=\langle v,w\rangle\leq\operatorname{SL}_{2}(K) and an involution u=(vZ,vZ)PSL2(K)2CG((24)g)u=(vZ,vZ)\in{\rm PSL}_{2}(K)^{2}\leq C_{G}((2^{4})_{g}) with CPSL2(K)2.y(u)=T2.(wZ,1),(1,wZ),yT2.D8C_{{\rm PSL}_{2}(K)^{2}.y}(u)=T_{2}.\langle(wZ,1),(1,wZ),y\rangle\cong T_{2}.D_{8}, where yy swaps the two factors PSL2(K){\rm PSL}_{2}(K). For the group (26)g=(25)e,u(2^{6})_{g}=\langle(2^{5})_{e},u\rangle we can choose u=u1:u2SL2(K)2SL2(K)CG(F0,0,1,1)u=u_{1}{:}u_{2}\in\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)\leq C_{G}(F_{0,0,1,1}) with each |ui|=4|u_{i}|=4, and the outside 2 of (SL2(K)2SL2(K)).2(\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)).2 centralises uu. If [vi,wi]=I2[v_{i},w_{i}]=-I_{2} for some wiSL2(K)w_{i}\in\operatorname{SL}_{2}(K), then w1:w2w_{1}{:}w_{2} also centralises uu, so CG((26)g)=24×T2.22C_{G}((2^{6})_{g})=2^{4}\times T_{2}.2^{2}.

  • (Case 2c)

    Suppose E𝒳2{(26)f}E\in\mathcal{X}_{2}\setminus\{(2^{6})_{f}\}. First, consider E=(24)iE=(2^{4})_{i}, so that U=(23)eU=(2^{3})_{e} and CG(E)C_{G}(E) has dimension 77. In addition, CG(U)=23×PSO6(K).γ=23×PSL4(K).γC_{G}(U)=2^{3}\times\operatorname{PSO}_{6}(K).\gamma=2^{3}\times{\rm PSL}_{4}(K).\gamma, where γ\gamma induces a graph automorphism on PSL4(K){\rm PSL}_{4}(K). Let g=γg=\gamma and w=diag(I2,I2)SL4(K)w=\operatorname{diag}(-I_{2},I_{2})\in\operatorname{SL}_{4}(K), so CSL4(K)(w)=T12(SL2(K)×SL2(K))C_{\operatorname{SL}_{4}(K)}(w)=T_{1}\circ_{2}(\operatorname{SL}_{2}(K)\times\operatorname{SL}_{2}(K)) and, by [21, Tables 4.3.1–4.3.3], we have CPSL4(K)(v)=(T1SL2(K)2SL2(K)).xC_{{\rm PSL}_{4}(K)}(v)=(T_{1}\circ\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)).x, where v=wZv=wZ, and xx inverts T1T_{1} and interchanges the two factors of SL2(K)2SL2(K)\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K). Note that we may take xx to be the permutation matrix corresponding to (1,3)(2,4)(1,3)(2,4), so that [x,g]=1=[w,g][x,g]=1=[w,g], and hence CPSL4(K).g(v)=(T1SL2(K)2SL2(K)).x.gC_{{\rm PSL}_{4}(K).g}(v)=(T_{1}\circ\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K)).x.g. Since gg stabilises each SL2(K)\operatorname{SL}_{2}(K), we have that gg induces an inner automorphism on SL2(K)\operatorname{SL}_{2}(K); by replacing gg by gygy for some y=y1:y2SL2(K)2SL2(K)y=y_{1}{:}y_{2}\in\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K), we may suppose that gg centralises each SL2(K)\operatorname{SL}_{2}(K). Note that we may suppose [y,x]=1[y,x]=1, hence [gy,x]=1[gy,x]=1, thus T1.g=T1.2T_{1}.g=T_{1}.2 where the outside 2 inverts T1T_{1}. Since dimCPSL4(K).g(v)=7\dim C_{{\rm PSL}_{4}(K).g}(v)=7, we may suppose u=vu=v, and hence E=U,vE=\langle U,v\rangle with

    CG(E)=CG((24)i)=23×((T1.i)2SO4(K)).x,C_{G}(E)=C_{G}((2^{4})_{i})=2^{3}\times((T_{1}.i)\circ_{2}\operatorname{SO}_{4}(K)).x,

    where xx commutes with ii, inverts T1T_{1}, and interchanges the two factors of SO4(K)=SL2(K)2SL2(K)\operatorname{SO}_{4}(K)=\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K).

    Now let E=(25)jE=(2^{5})_{j}, so that dimCG(E)=3\dim C_{G}(E)=3, and let U=(24)iU=(2^{4})_{i} with CG(U)C_{G}(U) given three lines above. By Figure 1 and Table 6, we have (25)i=U,z(2^{5})_{i}=\langle U,z\rangle for some involution zCG(U)z\in C_{G}(U) and dimCG((25)i)=3\dim C_{G}((2^{5})_{i})=3. In particular, it follows from Table 6 that (25)i(2^{5})_{i} and (25)j(2^{5})_{j} are the only subgroups of size 252^{5} whose centralisers have dimension 3. Thus, CG(U)C_{G}(U) contains exactly two involutions whose centralisers have dimension 3; we now construct two such centralisers. In the following we identity SO4(K)=SL2(K)2SL2(K)\operatorname{SO}_{4}(K)=\operatorname{SL}_{2}(K)\circ_{2}\operatorname{SL}_{2}(K).

    Note that CT1.i(x)=(T1)(2),i=22C_{T_{1}.i}(x)=\langle(T_{1})_{(2)},i\rangle=2^{2} and CSO4(K)(x)=2×PSL2(K)C_{\operatorname{SO}_{4}(K)}(x)=2\times{\rm PSL}_{2}(K), where 2=I2:I2SO4(K)2=-I_{2}{:}I_{2}\in\operatorname{SO}_{4}(K), thus

    C((T1.i)2SO4(K)).x(x)=222(I2:I2,x×PSL2(K))=23×PSL2(K),C_{((T_{1}.i)\circ_{2}\operatorname{SO}_{4}(K)).x}(x)=2^{2}\circ_{2}(\langle-I_{2}{:}I_{2},x\rangle\times{\rm PSL}_{2}(K))=2^{3}\times\operatorname{PSL}_{2}(K),

    and so CCG(U)(x)=26×PSL2(K)C_{C_{G}(U)}(x)=2^{6}\times{\rm PSL}_{2}(K). Let t=diag(s,s1):diag(s,s1)SO4(K)t=\operatorname{diag}(s,s^{-1}){:}\operatorname{diag}(s,s^{-1})\in\operatorname{SO}_{4}(K), where |s|=4|s|=4. So |t|=2|t|=2, [t,x]=1[t,x]=1, and CSO(K)(t)=(T12T1).(j:j)C_{\operatorname{SO}(K)}(t)=(T_{1}\circ_{2}T_{1}).(j{:}j) with jj acting via inversion (see [21, Tables 4.3.1–4.3.3]). Note that [j:j,x]=1[j{:}j,x]=1 and [t,x]=1[t,x]=1, so

    C((T1.i)2SO4(K)).x(t)=(T1.i)2(T12T1).(j:j).x=T3.23.C_{((T_{1}.i)\circ_{2}\operatorname{SO}_{4}(K)).x}(t)=(T_{1}.i)\circ_{2}(T_{1}\circ_{2}T_{1}).(j{:}j).x=T_{3}.2^{3}.

    In particular, CG(E)G{26×PSL2(K),23×T3.23}C_{G}(E)\in_{G}\{2^{6}\times{\rm PSL}_{2}(K),2^{3}\times T_{3}.2^{3}\}. If CG(E)=23×T3.23C_{G}(E)=2^{3}\times T_{3}.2^{3}, then OutG(E)\operatorname{Out}_{G}(E) stabilises CG(E)=T3C_{G}(E)^{\circ}=T_{3}, and so it also stabilises (T3)(2)=23(T_{3})_{(2)}=2^{3}. Thus OutG(E)\operatorname{Out}_{G}(E) is a subgroup of the parabolic subgroup OutSL6(2)(23)<Out(26)\operatorname{Out}_{\operatorname{SL}_{6}(2)}(2^{3})<\operatorname{Out}(2^{6}). This is impossible, since OutG(E)=24:Sp4(2)\operatorname{Out}_{G}(E)=2^{4}{:}\operatorname{Sp}_{4}(2), see Table 6. In conclusion, CG(E)=CG((25)j)=26×PSL2(K)C_{G}(E)=C_{G}((2^{5})_{j})=2^{6}\times{\rm PSL}_{2}(K), and so CG((25)i)=23×T3.23C_{G}((2^{5})_{i})=2^{3}\times T_{3}.2^{3}.

  • (Case 3)

    Let E=(26)fE=(2^{6})_{f}, so that dimCG(E)=0\dim C_{G}(E)=0, and let U=(25)fU=(2^{5})_{f} with CG(U)=22×T4.23C_{G}(U)=2^{2}\times T_{4}.2^{3}. Let uT4.23T4u\in T_{4}.2^{3}\setminus T_{4} be acting via inversion on T4T_{4}, so that CT4.23(u)=(T4)(2).23=24.23=25.22C_{T_{4}.2^{3}}(u)=(T_{4})_{(2)}.2^{3}=2^{4}.2^{3}=2^{5}.2^{2}. Now Table 6 implies that CG(E)=22×24.23C_{G}(E)=2^{2}\times 2^{4}.2^{3}. ∎

6.8. Proof of Proposition 6.3 for G=E8(K)G=E_{8}(K).

Yu [41, §8] has classified all elementary abelian 22-subgroups of GG, see Appendix B.1 for details and group labels; the non-toral groups are listed in Table 7. The structure of the corresponding normaliser quotients is also determined in [41], see Appendix B.2 for details. In the following we determine the structure of the centralisers.

Preliminary subgroups. By [21, Tables 4.3.1–4.3.3], there is an involution zGz\in G whose centraliser is CG(z)=SL2(K)2HC_{G}(z)=\operatorname{SL}_{2}(K)\circ_{2}H, where

H=E7,sc and L=H/Z(H)=E7,ad.H=E_{7,{\text{\rm sc}}}\quad\text{ and }\quad L=H/Z(H)=E_{7,{\text{\rm ad}}}.

Note that Hσ=E7,sc(q)HH^{\sigma}=E_{7,{\text{\rm sc}}}(q)\leq H for a suitable Steinberg morphism σ\sigma; by [4, Lemma 6.3], the group HσH^{\sigma} has subgroups 𝐐2,𝐐𝟑,𝐐4Q8{\bf Q}_{2},{\bf Q_{3}},{\bf Q}_{4}\cong Q_{8} such that

CHσ(𝐐2)\displaystyle C_{H^{\sigma}}({\bf Q}_{2}) =Z(H)×F4(q),\displaystyle=Z(H)\times F_{4}(q),
CHσ(𝐐3)\displaystyle C_{H^{\sigma}}({\bf Q}_{3}) =Z(H)×PSp8(q),\displaystyle=Z(H)\times{\rm PSp}_{8}(q),
CHσ(𝐐4)\displaystyle C_{H^{\sigma}}({\bf Q}_{4}) =Z(H)×(PΩ8+(q).22)\displaystyle=Z(H)\times({\rm P}\Omega_{8}^{+}(q).2^{2})

We fix this notation in the following and write 𝐐j=xj,yj{\bf Q}_{j}=\langle x_{j},y_{j}\rangle for j{2,3,4}j\in\{2,3,4\}, so that each xj2=yj2=zx_{j}^{2}=y_{j}^{2}=z.

We first determine CH(𝐐i)C_{H}({\bf Q}_{i}). The proof of [4, Lemma 6.2] yields Or(CHσ(x2))=E6ϵ(q)O^{r}(C_{H^{\sigma}}(x_{2}))=E^{\epsilon}_{6}(q). Note that CHσ(x2)CH(x2)C_{H^{\sigma}}(x_{2})\leq C_{H}(x_{2}) and y2Z(H)CL(x2Z(H))y_{2}Z(H)\in C_{L}(x_{2}Z(H)). It follows from [21, Tables 4.3.1–4.3.3] that CH(x2)=T13E6,sc(K)C_{H}(x_{2})=T_{1}\circ_{3^{*}}E_{6,{\text{\rm sc}}}(K), and y2=(i:γ)y_{2}=(i{:}\gamma) acts on T13E6,sc(K)T_{1}\circ_{3^{*}}E_{6,{\text{\rm sc}}}(K). Thus

CH(𝐐2)=2×CE6,sc(K)(γ).C_{H}({\bf Q}_{2})=2\times C_{E_{6,{\text{\rm sc}}}(K)}(\gamma).

By [21, Tables 4.3.1–4.3.3], we have CE6,sc(K)(γ){F4(K),PSp8(K)}C_{E_{6,{\text{\rm sc}}}(K)}(\gamma)\in\{F_{4}(K),{\rm PSp}_{8}(K)\}; moreover, we deduce from CHσ(𝐐2)=2×F4(q)C_{H^{\sigma}}({\bf Q}_{2})=2\times F_{4}(q) that CH(𝐐2)=Z(H)×F4(K)C_{H}({\bf Q}_{2})=Z(H)\times F_{4}(K); similarly, CH(𝐐3)=Z(H)×PSp8(K)C_{H}({\bf Q}_{3})=Z(H)\times{\rm PSp}_{8}(K) follows. Lastly, note that CH(x4)=SL8(K)/2C_{H}(x_{4})=\operatorname{SL}_{8}(K)/2 and y4=γy_{4}=\gamma acts on SL8(K)/2\operatorname{SL}_{8}(K)/2. Since CHσ(𝐐4)=2×(PΩ8+(q).22)CH(𝐐4)C_{H^{\sigma}}({\bf Q}_{4})=2\times({\rm P}\Omega_{8}^{+}(q).2^{2})\leq C_{H}({\bf Q}_{4}), it follows from [21, Tables 4.3.1–4.3.3] that CH(𝐐4)=Z(H)×PΩ8(K)C_{H}({\bf Q}_{4})=Z(H)\times{\rm P}\Omega_{8}(K).

Now let

P=u,vSL2(K)CG(z)P=\langle u,v\rangle\leq\operatorname{SL}_{2}(K)\leq C_{G}(z)

such that PQ8P\cong Q_{8} with u2=z=v2u^{2}=z=v^{2}. Each Yj=z,uxj,vyjY_{j}=\langle z,ux_{j},vy_{j}\rangle has type 232^{3} and satisfies

CG(Y2)\displaystyle C_{G}(Y_{2}) =CCG(z)(Y2)=23×F4(K),\displaystyle=C_{C_{G}(z)}(Y_{2})=2^{3}\times F_{4}(K),
CG(Y3)\displaystyle C_{G}(Y_{3}) =CCG(z)(Y3)=23×PSp8(K),\displaystyle=C_{C_{G}(z)}(Y_{3})=2^{3}\times{\rm PSp}_{8}(K),
CG(Y4)\displaystyle C_{G}(Y_{4}) =CCG(z)(Y4)=23×PΩ8+(K).\displaystyle=C_{C_{G}(z)}(Y_{4})=2^{3}\times{\rm P}\Omega_{8}^{+}(K).

In particular, each YjY_{j} is non-toral, and the dimensions listed in Table 7 determine

Y2=G(23)a,Y3=G(23)b,Y4=G(23)c.Y_{2}=_{G}(2^{3})_{a},\quad Y_{3}=_{G}(2^{3})_{b},\quad Y_{4}=_{G}(2^{3})_{c}.

A correspondence. We now show a correspondence between non-toral subgroups of G=E8(K)G=E_{8}(K) and non-toral subgroups of L=E7,ad(K)L=E_{7,{\text{\rm ad}}}(K). First, consider an elementary abelian subgroup

E=(23)x×UG,E=(2^{3})_{x}\times U\leq G,

where x{a,b,c}x\in\{a,b,c\} and UCG((23)x){F4(K),PSp8(K),PΩ8(K)}U\leq C_{G}((2^{3})_{x})^{\circ}\in\{F_{4}(K),{\rm PSp}_{8}(K),{\rm P}\Omega_{8}(K)\}. Note that EE is non-toral, and CG((23)x)=CL((22)x)C_{G}((2^{3})_{x})^{\circ}=C_{L}((2^{2})_{x})^{\circ} by Table 6. Recall from the previous paragraph that P=u,vSL2(K)P=\langle u,v\rangle\leq\operatorname{SL}_{2}(K) and define

M=P2HCG(z)=SL2(K)2H,M=P\circ_{2}H\leq C_{G}(z)=\operatorname{SL}_{2}(K)\circ_{2}H,

so that EME\leq M. If Z=zZ=\langle z\rangle, then ZEZ\leq E and M/Z=P/Z×H/Z=22×LM/Z=P/Z\times H/Z=2^{2}\times L. If π\pi denotes the projection from M/ZM/Z onto LL, then X=π(E/Z)=(22)x×UX=\pi(E/Z)=(2^{2})_{x}\times U and XE/ZX\cong E/Z. In particular, XX is a non-toral elementary abelian subgroup of LL and

CG(E)=(23)x×CCL((22)x)(U).C_{G}(E)=(2^{3})_{x}\times C_{C_{L}((2^{2})_{x})^{\circ}}(U).

Conversely, if x{a,b,c}x\in\{a,b,c\} and X=(22)x×ULX=(2^{2})_{x}\times U\leq L is an elementary abelian subgroup. Then XX is non-toral, UCL((22)x)U\leq C_{L}((2^{2})_{x})^{\circ} is elementary abelian, and E=(23)x×UGE=(2^{3})_{x}\times U\leq G is non-toral with X=π(E/Z)X=\pi(E/Z).

The following lemma will be useful.

Lemma 6.7.

With the previous notation, OutL(X)COutG(E)(z)\operatorname{Out}_{L}(X)\leq C_{\operatorname{Out}_{G}(E)}(z).

Proof.

Since M/Z=22×LM/Z=2^{2}\times L, we have CM/Z(E/Z)=22×CL(X)C_{M/Z}(E/Z)=2^{2}\times C_{L}(X) and NM/Z(E/Z)=22×NL(X)N_{M/Z}(E/Z)=2^{2}\times N_{L}(X), so OutL(X)=OutM/Z(E/Z)\operatorname{Out}_{L}(X)=\operatorname{Out}_{M/Z}(E/Z). Note that CG(E)CG((23)x)MC_{G}(E)\leq C_{G}((2^{3})_{x})\leq M, so CG(E)=CM(E)C_{G}(E)=C_{M}(E) and

OutM(E)=NM(E)/CM(E)OutG(E).\operatorname{Out}_{M}(E)=N_{M}(E)/C_{M}(E)\leq\operatorname{Out}_{G}(E).

Moreover, OutM/Z(E/Z)=OutM(E)\operatorname{Out}_{M/Z}(E/Z)=\operatorname{Out}_{M}(E) since NM/Z(E/Z)=NM(E)/ZN_{M/Z}(E/Z)=N_{M}(E)/Z. Now MCG(z)M\leq C_{G}(z) shows that OutL(X)=OutM/Z(E/Z)=OutM(E)COutG(E)(z)\operatorname{Out}_{L}(X)=\operatorname{Out}_{M/Z}(E/Z)=\operatorname{Out}_{M}(E)\leq C_{\operatorname{Out}_{G}(E)}(z). ∎

The column labelled “XLX\leq L” in Table 7 lists the subgroup XX specified by the name given in Table 6.

Centralisers. There are subgroups with names (23)a(2^{3})_{a}, (24)b(2^{4})_{b}, etc.  in LL and in GG, respectively; in the following, we write “G\leq G” and “L\leq L” to indicate which subgroup is meant.

Let E=(23)x×UGE=(2^{3})_{x}\times U\leq G be as in the previous paragraph, so that X=π(E/Z)=(22)x×UX=\pi(E/Z)=(2^{2})_{x}\times U is a non-toral subgroup of LL. Note that dimCG(E)=dimCL(X)=dimCCL((22)x)(U)\dim C_{G}(E)=\dim C_{L}(X)=\dim C_{C_{L}((2^{2})_{x})^{\circ}}(U), and dimCG(E)\dim C_{G}(E) is listed in Table 7 and dimCL(X)\dim C_{L}(X) is given in Table 9. In most of the cases, XX is uniquely determined by dimCG(E)\dim C_{G}(E), and so we can identify UU, therefore determining CG(E)=(23)x×CCL((22)x)(U)C_{G}(E)=(2^{3})_{x}\times C_{C_{L}((2^{2})_{x})^{\circ}}(U). For example, if E=(24)eGE=(2^{4})_{e}\leq G, then dimCG(E)=12\dim C_{G}(E)=12, so X23X\cong 2^{3} and dimCL(X)=12\dim C_{L}(X)=12. Now Table 9 implies that X=(23)fLX=(2^{3})_{f}\leq L with CL(X)=22×(SO4(K)2SO4(K)).22)C_{L}(X)=2^{2}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K)).2^{2}), hence

CG(E)=23×(SO4(K)2SO4(K)).22.C_{G}(E)=2^{3}\times(\operatorname{SO}_{4}(K)\circ_{2}\operatorname{SO}_{4}(K)).2^{2}.

Similar proofs work for the subgroups of GG in Table 7 that are not in

𝒳={(25)c,(25)g,(25)i,(26)b,(26)c,(26)e,(26)f,(26)g,(27)b,(27)d,(27)f,(28)a,(28)b}.\mathcal{X}=\{(2^{5})_{c},(2^{5})_{g},(2^{5})_{i},(2^{6})_{b},(2^{6})_{c},(2^{6})_{e},(2^{6})_{f},(2^{6})_{g},(2^{7})_{b},(2^{7})_{d},(2^{7})_{f},(2^{8})_{a},(2^{8})_{b}\}.

In the following we suppose that E=(23)x×UGE=(2^{3})_{x}\times U\leq G with X=22×ULX=2^{2}\times U\leq L, but XX cannot be determined uniquely by the dimension of CG(E)C_{G}(E); this includes the groups in 𝒳{(25)i}\mathcal{X}\setminus\{(2^{5})_{i}\}.

Note that if E=(28)aGE=(2^{8})_{a}\leq G, then its normaliser structure and [22, Table 1] show that EE is maximal non-toral and CG(E)=28C_{G}(E)=2^{8}. According to Table 9, the only other non-toral 27L2^{7}\leq L with centraliser of dimension 0 are (27)b,(27)dL(2^{7})_{b},(2^{7})_{d}\leq L, both with centralisers isomorphic to 282^{8}. However, (27)dL(2^{7})_{d}\leq L has no (22)xL(2^{2})_{x}\leq L as subgroups; this determines the centralisers of (28)a,(28)bG(2^{8})_{a},(2^{8})_{b}\leq G.

Now let E𝒳{(25)i,(28)a,(28)b}E\in\mathcal{X}\setminus\{(2^{5})_{i},(2^{8})_{a},(2^{8})_{b}\}. Recall that E=(23)x×UE=(2^{3})_{x}\times U with UCG((23)x)=CL((22)x)U\leq C_{G}((2^{3})_{x})^{\circ}=C_{L}((2^{2})_{x})^{\circ}; in particular, (23)xGE(2^{3})_{x}\leq_{G}E and so (22)xX(2^{2})_{x}\leq X. We now use Lemma 6.7 to determine XLX\leq L and so CG(E)C_{G}(E).

For example, if E=(25)gGE=(2^{5})_{g}\leq G, then dimCG(E)=10\dim C_{G}(E)=10, and Figure 9 shows that X24X\cong 2^{4} is one of (24)a,(24)fL(2^{4})_{a},(2^{4})_{f}\leq L. As subgroups of LL, we know that (22)aL(24)aL(2^{2})_{a}\leq_{L}(2^{4})_{a}\leq L and (22)aL(24)fL(2^{2})_{a}\not\leq_{L}(2^{4})_{f}\leq L. By Table 7, a Sylow 33-subgroup of OutG(E)=24:SO4(2)=24:Sym5\operatorname{Out}_{G}(E)=2^{4}{:}\operatorname{SO}^{-}_{4}(2)=2^{4}{:}\operatorname{Sym}_{5} has order 33. If X=(24)aLX=(2^{4})_{a}\leq L, then OutL(X)=Sym3×Sym3\operatorname{Out}_{L}(X)=\operatorname{Sym}_{3}\times\operatorname{Sym}_{3}, which is impossible by Lemma 6.7; thus X=(24)fLX=(2^{4})_{f}\leq L. Note that CL(X)=24×PSp4(K)C_{L}(X)=2^{4}\times{\rm PSp}_{4}(K), so CG(E)=CG((25)g)=25×PSp4(K)C_{G}(E)=C_{G}((2^{5})_{g})=2^{5}\times{\rm PSp}_{4}(K) is determined. If E=(25)cGE=(2^{5})_{c}\leq G, then dimCG(E)=10\dim C_{G}(E)=10, and so X=(24)aLX=(2^{4})_{a}\leq L; this determines CG(E)=CG((25)c)23×(T1×GL3(K)).2C_{G}(E)=C_{G}((2^{5})_{c})2^{3}\times(T_{1}\times\operatorname{GL}_{3}(K)).2. In a similar way, Lemma 6.7 can be used to identify the subgroups XX for the pairs ((27)b,(27)d)G((2^{7})_{b},(2^{7})_{d})\subseteq G and ((26)b,(26)g)G((2^{6})_{b},(2^{6})_{g})\subseteq G. Lemma 6.7 also helps to identify XX for ((26)e,(26)f)G((2^{6})_{e},(2^{6})_{f})\subseteq G: if E=(26)fE=(2^{6})_{f}, then Table 10 shows that OutG(E)=25:SO5(2)\operatorname{Out}_{G}(E)=2^{5}{:}\operatorname{SO}_{5}(2) centralises an involution uEu\in E; if u=Gzu=_{G}z, then

OutG(E)=OutCG(z)(E)=OutSL2(K)/Z(E/Z)×OutL(X),\operatorname{Out}_{G}(E)=\operatorname{Out}_{C_{G}(z)}(E)=\operatorname{Out}_{\operatorname{SL}_{2}(K)/Z}(E/Z)\times\operatorname{Out}_{L}(X),

which is impossible. Now set Y=z,u=22Y=\langle z,u\rangle=2^{2}; Lemma 6.7 shows that OutL(X)COutG(E)(Y)\operatorname{Out}_{L}(X)\leq C_{\operatorname{Out}_{G}(E)}(Y). Table 10 yields COutG(E)(Y)=24:(CSO5(2)(Y))24:SO5(2)C_{\operatorname{Out}_{G}(E)}(Y)=2^{4}{:}(C_{\operatorname{SO}_{5}(2)}(Y))\leq 2^{4}{:}\operatorname{SO}_{5}(2). Since |SO5(2)|=|Sym6|=24.32.5|\operatorname{SO}_{5}(2)|=|\operatorname{Sym}_{6}|=2^{4}.3^{2}.5, we deduce that OutL((25)f)\operatorname{Out}_{L}((2^{5})_{f}) is not a subgroup of COutG(E)(Y)C_{\operatorname{Out}_{G}(E)}(Y); hence X=(25)gLX=(2^{5})_{g}\leq L.

Let E=(27)fGE=(2^{7})_{f}\leq G; here XX is one of (26)c,(26)dL(2^{6})_{c},(2^{6})_{d}\leq L, but (26)cL(2^{6})_{c}\leq L has no non-toral (22)xL(2^{2})_{x}\leq L as a subgroup. This determines X=(26)dX=(2^{6})_{d}, hence CG(E)=27×PSL2(K)C_{G}(E)=2^{7}\times{\rm PSL}_{2}(K). Similarly, let E=(26)cGE=(2^{6})_{c}\leq G; here XX is one of (25)b,(25)i,(25)jL(2^{5})_{b},(2^{5})_{i},(2^{5})_{j}\leq L; however, (25)i,(25)jL(2^{5})_{i},(2^{5})_{j}\leq L have no (22)xL(2^{2})_{x}\leq L as subgroup. This determines X=(25)bLX=(2^{5})_{b}\leq L and CG(E)=CG((26)c)=26×PGL2(K)C_{G}(E)=C_{G}((2^{6})_{c})=2^{6}\times{\rm PGL}_{2}(K).

Lastly, consider EG(23)x×UE\neq_{G}(2^{3})_{x}\times U for all x{a,b,c}x\in\{a,b,c\}; it follows from Table 7 that E=(25)iGE=(2^{5})_{i}\leq G has distribution 2B312{\rm B}_{31}. It is shown in [30, Section 2] that M=25+10.SL5(2)M=2^{5+10}.\operatorname{SL}_{5}(2) is a maximal subgroup of GG, and R=Z(O2(M))=25R=Z(O_{2}(M))=2^{5} with CG(R)=O2(M)=25+10C_{G}(R)=O_{2}(M)=2^{5+10}. Thus, RR is non-toral and we determine R=GER=_{G}E, hence CG(E)=25+10C_{G}(E)=2^{5+10}.

The structure of the centralisers has the following corollary.

Corollary 6.8.

If E=(23)x×UE=(2^{3})_{x}\times U and X=(22)x×UX=(2^{2})_{x}\times U, and E=(23)y×UE^{\prime}=(2^{3})_{y}\times U^{\prime} and X=(22)y×UX^{\prime}=(2^{2})_{y}\times U^{\prime} for x,y{a,b,c}x,y\in\{a,b,c\}, then X=LXX=_{L}X^{\prime} if and only if E=GEE=_{G}E^{\prime}.

In conclusion, we have proved the following proposition, and the proof of Proposition 6.3 is complete.

Proposition 6.9.

If EE is as given in Table 7, then CG(E)C_{G}(E) is as given in that table.

Appendix A Details for E7,adE_{7,{\text{\rm ad}}} and p=2p=2

This section complements the results in Section 6.7.

A.1. The families of subgroups in [41]

Yu [41] has classified the subgroups of G=E7,ad(K)G=E_{7,{\text{\rm ad}}}(K), up to conjugacy, into the following families of subgroups. Families (1a)–(1d) below are the subgroups which contain an element from class 4H4{\rm H}, hence lie in the centraliser (E6(K)3T1).2(E_{6}(K)\circ_{3}T_{1}).2. Families (2a) and (2b) are those subgroups which contain an element of 4A4{\rm A} but no element of 4H4{\rm H}, hence lie in a subgroup (SL8(K)/4).2(\operatorname{SL}_{8}(K)/4).2 but not (E6(K)3T1).2(E_{6}(K)\circ_{3}T_{1}).2. The final two families (3a) and (3b) are those subgroups containing only involutions from class 2BC2{\rm BC}. For an elementary abelian 22-subgroup EE, let EBC=(E2BC){1}E_{{\rm BC}}=(E\cap 2{\rm B}{\rm C})\cup\{1\}; by [41, Lemma 7.3], this is a subgroup of EE, and E/EBCE/E_{{\rm BC}} has rank at most 22. A direct calculation with our algorithm from Section 5.1 shows that E/EBCE/E_{{\rm BC}} has rank at most 11 for toral subgroups. We can now state the families of subgroups.

  • (1a)

    Fr,sF_{r,s} (r2,s3)(r\leq 2,\ s\leq 3). These subgroups are described in [41, §5, §6, Lemma 7.6; Propositions 7.8(1) and 7.9]. They are precisely the subgroups containing a conjugate of (22)a(2^{2})_{a}, and are therefore all non-toral; this gives 1212 classes of non-toral subgroups. The rank of such a group EE is r+s+2r+s+2, and E/EBCE/E_{{\rm BC}} has rank 22.

  • (1b)

    Fr,sF_{r,s}^{\prime} (r2,s3)(r\leq 2,\ s\leq 3). These are described in [41, §6, Lemma 7.6; Propositions 7.8(2) and 7.9]. By definition these are subgroups of the form E×xE^{\prime}\times\left<x\right>, where CG(x)=(E6(K)3T1).2C_{G}(x)=(E_{6}(K)\circ_{3}T_{1}).2 with x4Hx\in 4{\rm H} for certain elementary abelian subgroups E<E6(K)E^{\prime}<E_{6}(K). Since xx lies in the T1T_{1} factor, such a subgroup is toral if and only if EE^{\prime} is toral in E6(K)E_{6}(K). From the classification for E6(K)E_{6}(K), it follows that the non-toral subgroups here are precisely the three groups with s=3s=3. The rank of a subgroup EE in each case is r+s+1r+s+1, and E/EBCE/E_{{\rm BC}} has rank 11.

  • (1c)

    Fϵ,δ,r,sF_{\epsilon,\delta,r,s} (ϵ+δ1,r+s2)(\epsilon+\delta\leq 1,\ r+s\leq 2). These are described in [41, Propositions 2.24, 2.29, 7.8(3), and 7.9; Definition 2.27; Lemma 7.6]. Such a subgroup EE has rank ϵ+2δ+r+2s+2\epsilon+2\delta+r+2s+2 and E/EBCE/E_{{\rm BC}} has rank 22, hence all 1818 of these subgroups are non-toral. We take this opportunity to point out an error in the stated definition in [41, p. 273]; correcting this error, the definition of Fϵ,δ,r,sF_{\epsilon,\delta,r,s} in [41, p. 278] is

    Fϵ,δ,r,s={σ2,x0,x1,,xϵ+2δ,x3,,x2+r+2s:(r,s)(2,0),σ2,x0,x1,,xϵ+2δ,x3,x5:(r,s)=(2,0).\displaystyle\hskip 25.83325ptF_{\epsilon,\delta,r,s}=\left\{\begin{array}[]{ll}\left<\sigma_{2},x_{0},x_{1},\ldots,x_{\epsilon+2\delta},x_{3},\ldots,x_{2+r+2s}\right>&\colon(r,s)\neq(2,0),\\ \left<\sigma_{2},x_{0},x_{1},\ldots,x_{\epsilon+2\delta},x_{3},x_{5}\right>&\colon(r,s)=(2,0).\end{array}\right.

    where the elements xix_{i} are also defined in [41, p. 273]. With this corrected definition the remaining results in [41] regarding these groups are correct as stated.111We thank Dr. Yu for clarifying this.

  • (1d)

    Fϵ,δ,r,sF_{\epsilon,\delta,r,s}^{\prime} (ϵ+δ1,r+s2,s1)(\epsilon+\delta\leq 1,\ r+s\leq 2,\ s\geq 1). These subgroups all have the form E×xE^{\prime}\times\left<x\right> where CG(x)=(E6(K)3T1).2C_{G}(x)=(E_{6}(K)\circ_{3}T_{1}).2 with xT1x\in T_{1} and EPSp8(K)E6(K)E^{\prime}\leq\operatorname{PSp}_{8}(K)\leq E_{6}(K). Each subgroup EE^{\prime} is toral in E6(K)E_{6}(K) as the non-toral subgroups of E6(K)E_{6}(K) lie in the class also labelled Fr,sF_{r,s}^{\prime} in [41, p. 272]. Thus all subgroups in this class are toral.

  • (2a)

    Fr,s′′F_{r,s}^{\prime\prime} (r+s3)(r+s\leq 3). This family is described in [41, Proposition 7.14]. They are the elementary abelian subgroups EE with Dist(E)=2BCa4Ab\operatorname{Dist}(E)=2{\rm BC}_{a}4{\rm A}_{b} with a0a\geq 0 and b>0b>0, and Rank(E/EBC)=1\operatorname{Rank}(E/E_{{\rm BC}})=1. The rank of such a subgroup is r+2s+1r+2s+1, and it follows that Dist(E)=2BCa14Aa\operatorname{Dist}(E)=2{\rm BC}_{a-1}4{\rm A}_{a} where a=2r+2s=|EBC|a=2^{r+2s}=|E_{{\rm BC}}|. Using the algorithm of Section 5.1, we see that there are four toral such subgroups, with respective distributions 4A14{\rm A}_{1}, 2BC14A22{\rm BC}_{1}4{\rm A}_{2}, 2BC34A42{\rm BC}_{3}4{\rm A}_{4}, and 2BC74A82{\rm BC}_{7}4{\rm A}_{8}. From the description of the groups and their generators given in [41, p. 280], the subgroups Fr,0′′F_{r,0}^{\prime\prime} are visibly toral, and thus the remaining six subgroups are non-toral.

  • (2b)

    FrF_{r}^{\prime} (r3)(r\leq 3). These are also described in [41, Proposition 7.14], and are precisely the elementary abelian subgroups EE with Dist(E)=2BCa4Ab\operatorname{Dist}(E)=2{\rm BC}_{a}4{\rm A}_{b} with a0a\geq 0 and b>0b>0, and Rank(E/EBC)=2\operatorname{Rank}(E/E_{{\rm BC}})=2. It follows at once that all four such subgroups are non-toral, the rank of such a subgroup is r+2r+2, and its distribution is 2BC2r14A32r2{\rm BC}_{2^{r}-1}4{\rm A}_{3\cdot 2^{r}}. We have F0F1F2F3F_{0}^{\prime}\leq F_{1}^{\prime}\leq F_{2}^{\prime}\leq F_{3}^{\prime}.

  • (3a)

    Fr,s′′′F_{r,s}^{\prime\prime\prime} (r+s3)(r+s\leq 3). The containment relations Fϵ+r,δ+s′′′Fϵ,δ,r,sF_{\epsilon+r,\delta+s}^{\prime\prime\prime}\leq F_{\epsilon,\delta,r,s}^{\prime} stated in [41, Remark 7.27] show that these 99 subgroups are always toral.

  • (3b)

    Fr′′F_{r}^{\prime\prime} (r2)(r\leq 2). These are described in [41, Proposition 7.22]. These are precisely the subgroups EBCE_{{\rm BC}} where EE is one of the subgroups Fr,3F_{r,3} above. Our algorithm from Section 5.1 finds exactly 1010 toral 2BC2{\rm BC}-pure subgroups, which are necessarily the toral 2BC2{\rm BC}-pure subgroups Fr,s′′′F_{r,s}^{\prime\prime\prime} above. Hence the three subgroups Fr′′F_{r}^{\prime\prime} are all non-toral. We have Rank(Fr′′)=Rank(Fr,3)2=r+3\operatorname{Rank}(F_{r}^{\prime\prime})=\operatorname{Rank}(F_{r,3})-2=r+3 and Fr′′Fr,3F_{r}^{\prime\prime}\leq F_{r,3}^{\prime}, see [41, p. 284].

This provides us with 12+3+18+6+4+3=4612+3+18+6+4+3=46 classes of non-toral subgroups, as expected. From their definition, we see that the subgroups Fr,sF_{r,s} are ordered by Fr1,s1Fr2,s2F_{r_{1},s_{1}}\leq F_{r_{2},s_{2}} if and only if r1r2r_{1}\leq r_{2} and s1s2s_{1}\leq s_{2}, and similarly for the Fr,sF_{r,s}^{\prime}. It is easy to see when the various subgroups Fϵ,δ,r,sF_{\epsilon,\delta,r,s} are contained in one another, from their definition. The remaining distributions can be calculated from [41, Proposition 7.9], combined with the knowledge of |EBC||E_{{\rm BC}}|. Specifically, if EE has rank aa and EBCE_{{\rm BC}} has rank bb, then Dist(E)=2BC2b14Ax4Hy\operatorname{Dist}(E)=2{\rm BC}_{2^{b}-1}4{\rm A}_{x}4{\rm H}_{y} where x+y=2a2bx+y=2^{a}-2^{b} and yxy-x is the defect defe(E)\operatorname{defe}(E), as defined in [41, Definition 7.2] and calculated in [41, Proposition 7.9]. Hence y=12(2a2b+defe(E))y=\frac{1}{2}\left(2^{a}-2^{b}+\operatorname{defe}(E)\right) and x=12(2a2bdefe(E))x=\frac{1}{2}\left(2^{a}-2^{b}-\operatorname{defe}(E)\right).

A.2. Normaliser quotients

The structure of NG(E)/CG(E)N_{G}(E)/C_{G}(E) for the various subgroups EE is stated in [41, Proposition 7.26]. We now unravel some of the notation there. The notation P(r,s,𝔽2)P(r,s,\mathbb{F}_{2}) means the group of block-upper-triangular matrices in GLr+s(2)\operatorname{GL}_{r+s}(2) with blocks of size rr and ss (cf. [41, Proposition 5.5]); thus

P(r,s,𝔽2)2rs:(GLr(2)×GLs(2)).P(r,s,\mathbb{F}_{2})\cong 2^{rs}\mathpunct{:}(\operatorname{GL}_{r}(2)\times\operatorname{GL}_{s}(2)).

Also, Sp(s)\operatorname{Sp}(s) means Sp2s(2)\operatorname{Sp}_{2s}(2) in our notation, and the groups Sp(δ+s;ϵ)\operatorname{Sp}(\delta+s;\epsilon) are understood as the following matrix groups of degree 2δ+2s+ϵ+12\delta+2s+\epsilon+1:

Sp(δ+s;0)\displaystyle\operatorname{Sp}(\delta+s;0) =SO2δ+2s+1(2),\displaystyle=\operatorname{SO}_{2\delta+2s+1}(2),
Sp(δ+s;1)\displaystyle\operatorname{Sp}(\delta+s;1) =(1𝟎SO2δ+2s+1(2))22δ+2s:SO2δ+2s+1(2),\displaystyle=\begin{pmatrix}1&\ast\\ \mathbf{0}&\operatorname{SO}_{2\delta+2s+1}(2)\end{pmatrix}\cong 2^{2\delta+2s}\mathpunct{:}\operatorname{SO}_{2\delta+2s+1}(2),

with SO2δ+2s+1(2)\operatorname{SO}_{2\delta+2s+1}(2) (Sp2δ+2s(2)\cong\operatorname{Sp}_{2\delta+2s}(2)) in its natural orthogonal representation, and \ast indicates the (2δ+2s)(2\delta+2s)-dimensional symplectic module for SO2δ+2s+1(2)\operatorname{SO}_{2\delta+2s+1}(2), considered as a subspace of co-dimension 11 in the space of (2δ+2s+1)(2\delta+2s+1)-dimensional row vectors. This gives the structure for the normaliser quotients of the non-toral subgroups in these families, see Table 8. Here SLa(2)\operatorname{SL}_{a}(2), Spb(2)\operatorname{Sp}_{b}(2) etc. indicate that all matrices in these groups occur in the block, and \ast indicates that all matrices of the appropriate size occur in the block. For clarity, when dealing with the groups Sp(δ+s;ϵ)\operatorname{Sp}(\delta+s;\epsilon) we write n,m\ast_{n,m} to indicate the precise size of the blocks occurring. If some dimension is 0, then the corresponding rows and columns are omitted entirely.

Table 8. Normaliser quotients of the non-toral elementary abelian 22-subgroups of the algebraic group E7,adE_{7,{\text{\rm ad}}}
EE NG(E)/CG(E)N_{G}(E)/C_{G}(E)
Fr,sF_{r,s} (SLr(2)𝟎SLs(2)𝟎𝟎𝟎SL2(2))\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast&\ast\\ \mathbf{0}&\operatorname{SL}_{s}(2)&\mathbf{0}\\ \mathbf{0}&\mathbf{0}&\operatorname{SL}_{2}(2)\end{pmatrix}
Fϵ,δ,r,sF_{\epsilon,\delta,r,s} (SLr(2)r,ϵ+2δ+2s+1𝟎Sp(δ+s;ϵ)ϵ+2δ+2s+1,1𝟎𝟎1)\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast_{r,\epsilon+2\delta+2s+1}&\ast\\ \mathbf{0}&\operatorname{Sp}(\delta+s;\epsilon)&\ast_{\epsilon+2\delta+2s+1,1}\\ \mathbf{0}&\mathbf{0}&1\\ \end{pmatrix}
Fr,sF_{r,s}^{\prime} (SLr(2)𝟎SLs(2)𝟎𝟎𝟎1)\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast&\ast\\ \mathbf{0}&\operatorname{SL}_{s}(2)&\mathbf{0}\\ \mathbf{0}&\mathbf{0}&1\end{pmatrix}
Fr,s′′F_{r,s}^{\prime\prime} (SLr(2)𝟎Sp2s(2)𝟎𝟎1)\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast&\ast\\ \mathbf{0}&\operatorname{Sp}_{2s}(2)&\ast\\ \mathbf{0}&\mathbf{0}&1\end{pmatrix}
FrF_{r}^{\prime} (SLr(2)𝟎SL2(2))\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast\\ \mathbf{0}&\operatorname{SL}_{2}(2)\end{pmatrix}
Fr′′F_{r}^{\prime\prime} (SLr(2)𝟎SL3(2))\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast\\ \mathbf{0}&\operatorname{SL}_{3}(2)\end{pmatrix}

A.3. A direct computation of all non-toral subgroups

Recall from Section 6.7 that we can compute all elementary abelian subgroups of GG within the finite normalisers of the maximal non-toral 272^{7} and 282^{8}. In Tables 9(A) and (B) we list the elementary abelian 22-subgroups of the maximal non-toral 272^{7} and 282^{8}, respectively. Note that some groups occur twice because the computations have been done up to conjugacy in NG(27)N_{G}(2^{7}) and NG(28)N_{G}(2^{8}), respectively. We comment on the identification of the subgroups, using the notation introduced in [41]. Those subgroups named “toral” have been identified because they have a distribution unique to a toral subgroups, or they are computed as a subgroup of such a toral subgroup. Subgroups with distributions different to those of toral subgroups must be non-toral, and we use the notation of [41] (together with information on their distribution) to identify them. Below are the ad-hoc arguments which have been used in this identification. The complete Hasse diagram of non-toral subgroups is given in Figure 1; inclusions in that diagram are computed up to conjugacy in the normalisers.

Remark A.1.
  • (a)

    The Klein four-subgroups of GG and their distributions are given in [41, Table 3]. Our algorithm shows that all but three of these are toral; the non-toral ones are the subgroups Γ6\Gamma_{6}, Γ7\Gamma_{7}, Γ8\Gamma_{8}, which we denote (22)a(2^{2})_{a}, (22)b(2^{2})_{b}, (22)c(2^{2})_{c} in Table 6. Note that these are also precisely the Klein four-subgroups of EE of GG such that E/EBCE/E_{{\rm BC}} has rank 22.

  • (b)

    The group F0′′F_{0}^{\prime\prime} can be identified because there is no other non-toral subgroup in 272^{7} or 282^{8} with distribution 2BC7. Similarly F1′′F_{1}^{\prime\prime} is the only un-identified subgroup with distribution 2BC15, and F2′′F_{2}^{\prime\prime} is the only un-identified subgroup with distribution 2BC31.

  • (c)

    Group (33) in Tables 9(A) and group (27) in Table 9(B) are both subgroups of a copy of a non-toral F0,1,1,0F_{0,1,1,0}. If they are both toral, then there is no unidentified subgroup left with distribution 2BC7A8, which means the non-toral F1,1′′F_{1,1}^{\prime\prime} is missing. Hence F0,1,1,0F_{0,1,1,0} contains a copy of F1,1′′F_{1,1}^{\prime\prime}, which is non-toral, hence (33) in Table 9(A) and (27) in Table 9(B) have this type.

  • (d)

    Group (43) in Table 9(B) cannot be F2,1′′F_{2,1}^{\prime\prime} since otherwise we have missed out F0,0,1,1F_{0,0,1,1}; thus (43) is F0,0,1,1F_{0,0,1,1}. This implies that (52) in Table 9(A) must be F1,2F_{1,2}.

  • (e)

    If group (25) in Table 9(B) was a copy of F1,1′′F_{1,1}^{\prime\prime} then, because it is contained in F3F_{3}^{\prime} in the 282^{8}-lattice, we would also see F3>F1,1′′F_{3}^{\prime}>F_{1,1}^{\prime\prime} in the 272^{7}-lattice; since we only see F3>F2F_{3}^{\prime}>F_{2}^{\prime} there, we conclude that group (25) and its subgroup (13) are toral.

  • (f)

    Subgroup (13) in Table 9(B) is toral, so subgroups (21) in Table 9(A) and (16) in Table 9(B) are the only unidentified subgroups left with distribution 2BC3A4, so one is non-toral. They are each a subgroup of a copy of F0,1,0,0F_{0,1,0,0}, hence they are both non-toral and have type F0,1′′F_{0,1}^{\prime\prime}.

  • (g)

    Since group (41) in Table 9(B) contains a copy of F0,0,2,0F_{0,0,2,0} it must be F1,0,2,0F_{1,0,2,0}, as the only other subgroup with the same distribution is F1,0,0,1F_{1,0,0,1}, which does not contain such a subgroup. Since (42) does not contain F0,0,2,0F_{0,0,2,0} it must be F1,0,0,1F_{1,0,0,1}.

  • (h)

    Group (56) in Table 9(A) and group (52) in Table 9(B) must be F1,3F_{1,3} and F0,1,0,1F_{0,1,0,1}; since F1,3F_{1,3} is a subgroup of F2,3F_{2,3}, this forces that (56) is F1,3F_{1,3}.

  • (i)

    It remains to identify group (48) in Table (A), and groups (44) and (45) in Table (B). All three have distribution 2BC15A162{\rm B}{\rm C}_{15}{\rm A}_{16} and contain F1,1′′F_{1,1}^{\prime\prime}, and the only non-toral subgroups with this distribution that have not been found elsewhere are F2,1′′F_{2,1}^{\prime\prime} and F0,2′′F_{0,2}^{\prime\prime}. The groups (48) from (A) and (44) from (B) are each contained in a copy of F0,1,2,0F_{0,1,2,0}, while group (45) from (B) is not; hence the first two are GG-conjugate, and not conjugate to the third. Let AA be one of the subgroups contained in F0,1,2,0F_{0,1,2,0}, and let BB a subgroup from the other class. From the discussion in Case 2c) of Proposition 6.6 we have CG(A)=23×LC_{G}(A)=2^{3}\times L for L{23×PSL2(K),T3.23}L\in\{2^{3}\times{\rm PSL}_{2}(K),T_{3}.2^{3}\}, and thus F0,1,2,0=A,uF_{0,1,2,0}=\langle A,u\rangle for some involution uLu\in L. Table 6 now implies that dimCG(F0,1,2,0)=0\dim C_{G}(F_{0,1,2,0})=0, hence dimCL(u)=0\dim C_{L}(u)=0, and so L23×PSL2(K)L\neq 2^{3}\times{\rm PSL}_{2}(K) by [21, Tables 4.3.1–4.3.3]. It follows that A=F2,1′′A=F_{2,1}^{\prime\prime} and B=F0,2′′B=F_{0,2}^{\prime\prime}.

Table 9. Subgroups of maximal non-toral 272^{7} and 282^{8} in E7,adE_{7,{\text{\rm ad}}}; a name “toral” indicates that the group is toral because of its distribution, or is contained in such a group; a name “(toral)” indicates that the group has later been identified as toral.
(A) subgroups of 272^{7}
Dist Cent dim name
(1) 2BC1 69 toral
(2) 2BC1 69 toral
(3) 4H1 79 toral
(4) 4A1 63 toral
(5) 2BC3 37 toral
(6) 2BC3 37 toral
(7) 2BC14H2 47 toral
(8) 2BC14A2 31 toral
(9) 2BC3 37 toral
(10) 2BC14A14H1 39 toral
(11) 2BC14A2 31 toral
(12) 4H3 52 F0,0F_{0,0}
(13) 4A24H1 36 F0,0,0,0F_{0,0,0,0}
(14) 4A3 28 F0F_{0}^{\prime}
(15) 2BC7 21 toral
(16) 2BC7 21 toral
(17) 2BC34A24H2 23 toral
(18) 2BC34A4 15 toral
(19) 2BC7 21 F0′′F_{0}^{\prime\prime}
(20) 2BC34A34H1 19 toral
(21) 2BC34A4 15 F0,1′′F_{0,1}^{\prime\prime}
(22) 2BC14A34H3 24 F0,1F_{0,1}
(23) 2BC14A54H1 16 F1,0,0,0F_{1,0,0,0}
(24) 2BC14A6 12 F1F_{1}^{\prime}
(25) 2BC34A4 15 toral
(26) 2BC14A44H2 20 F0,0,1,0F_{0,0,1,0}
(27) 2BC14A6 12 F1F_{1}^{\prime}
(28) 2BC34H4 31 toral
(29) 2BC14H6 36 F1,0F_{1,0}
(30) 2BC15 13 toral
(31) 2BC15 13 F1′′F_{1}^{\prime\prime}
(32) 2BC74A64H2 11 toral
(33) 2BC74A8 7 F1,1′′F_{1,1}^{\prime\prime}
(34) 2BC74A74H1 9 F0,3F_{0,3}^{\prime}
(35) 2BC34A94H3 10 F0,2F_{0,2}
(36) 2BC34A114H1 6 F0,1,0,0F_{0,1,0,0}
(37) 2BC74A8 7 toral
(38) 2BC34A104H2 8 F1,0,1,0F_{1,0,1,0}
(39) 2BC34A12 4 F2F_{2}^{\prime}
(40) 2BC34A12 4 F2F_{2}^{\prime}
(41) 2BC74A44H4 15 toral
(42) 2BC34A64H6 16 F1,1F_{1,1}
(43) 2BC34A84H4 12 F0,0,2,0F_{0,0,2,0}
(44) 2BC34H12 28 F2,0F_{2,0}
(45) 2BC31 9 F2′′F_{2}^{\prime\prime}
(46) 2BC154A144H2 5 F1,3F_{1,3}^{\prime}
(47) 2BC74A214H3 3 F0,3F_{0,3}
(48) 2BC154A16 3 F2,1′′F_{2,1}^{\prime\prime}
(49) 2BC74A224H2 2 F0,1,1,0F_{0,1,1,0}
(50) 2BC74A24 0 F3F_{3}^{\prime}
(51) 2BC154A124H4 7 toral
(52) 2BC74A184H6 6 F1,2F_{1,2}
(53) 2BC74A204H4 4 F1,0,2,0F_{1,0,2,0}
(54) 2BC74A124H12 12 F2,1F_{2,1}
(55) 2BC314A284H4 3 F2,3F_{2,3}^{\prime}
(56) 2BC154A424H6 1 F1,3F_{1,3}
(57) 2BC154A444H4 0 F0,1,2,0F_{0,1,2,0}
(58) 2BC154A364H12 4 F2,2F_{2,2}
(59) 2BC314A844H12 0 F2,3F_{2,3}
(B) subgroups of 282^{8}
Dist Cent dim name
(1) 4A1 63 toral
(2) 2BC1 69 toral
(3) 4A1 63 toral
(4) 4H1 79 toral
(5) 2BC14A2 31 toral
(6) 4A3 28 F0F_{0}^{\prime}
(7) 4A24H1 36 F0,0,0,0F_{0,0,0,0}
(8) 2BC3 37 toral
(9) 2BC14A2 31 toral
(10) 2BC14H2 47 toral
(11) 2BC3 37 toral
(12) 2BC14A14H1 39 toral
(13) 2BC34A4 15 (toral)
(14) 2BC14A6 12 F1F_{1}^{\prime}
(15) 2BC14A44H2 20 F0,0,1,0F_{0,0,1,0}
(16) 2BC34A4 15 F0,1′′F_{0,1}^{\prime\prime}
(17) 2BC14A54H1 16 F1,0,0,0F_{1,0,0,0}
(18) 2BC7 21 toral
(19) 2BC34A4 15 toral
(20) 2BC7 21 toral
(21) 2BC34A24H2 23 toral
(22) 2BC34H4 31 toral
(23) 2BC34A34H1 19 toral
(24) 2BC34A14H3 27 toral
(25) 2BC74A8 7 (toral)
(26) 2BC34A12 4 F2F_{2}^{\prime}
(27) 2BC74A8 7 F1,1′′F_{1,1}^{\prime\prime}
(28) 2BC34104H2 8 F1,0,1,0F_{1,0,1,0}
(29) 2BC34A84H4 12 F0,0,2,0F_{0,0,2,0}
(30) 2BC34114H1 6 F0,1,0,0F_{0,1,0,0}
(31) 2BC34A94H3 10 F0,0,0,1F_{0,0,0,1}
(32) 2BC74A8 7 toral
(33) 2BC74A64H2 11 toral
(34) 2BC74A44H4 15 toral
(35) 2BC74A44H4 15 toral
(36) 2BC74A24H6 19 toral
(37) 2BC15 13 toral
(38) 2BC15 13 toral
(39) 2BC74A24 0 F3F_{3}^{\prime}
(40) 2BC74A224H2 2 F0,1,1,0F_{0,1,1,0}
(41) 2BC74A204H4 4 F1,0,2,0F_{1,0,2,0}
(42) 2BC74A204H4 4 F1,0,0,1F_{1,0,0,1}
(43) 2BC74A184H6 6 F0,0,1,1F_{0,0,1,1}
(44) 2BC154A16 3 F2,1′′F_{2,1}^{\prime\prime}
(45) 2BC154A16 3 F0,2′′F_{0,2}^{\prime\prime}
(46) 2BC154A124H4 7 toral
(47) 2BC154A104H6 9 toral
(48) 2BC154A84H8 11 toral
(49) 2BC154A64H10 13 toral
(50) 2BC31 9 toral
(51) 2BC154A444H4 0 F0,1,2,0F_{0,1,2,0}
(52) 2BC154A424H6 1 F0,1,0,1F_{0,1,0,1}
(53) 2BC154A404H8 2 F1,0,1,1F_{1,0,1,1}
(54) 2BC154A384H10 3 F0,0,0,2F_{0,0,0,2}
(55) 2BC314A32 1 F1,2′′F_{1,2}^{\prime\prime}
(56) 2BC314A204H12 7 toral
(57) 2BC314A164H16 9 toral
(58) 2BC63 7 toral
(59) 2BC314A844H12 0 F0,1,1,1F_{0,1,1,1}
(60) 2BC314A804H16 1 F1,0,0,2F_{1,0,0,2}
(61) 2BC634A64 0 F0,3′′F_{0,3}^{\prime\prime}
(62) 2BC634A364H28 7 toral
(63) 2BC634A1644H28 0 F0,1,0,2F_{0,1,0,2}
Figure 1. Hasse diagram of all non-toral 22-subgroups of E7,adE_{7,{{\text{\rm ad}}}}; cross-family inclusions in grey.
F0,1,0,2F_{0,1,0,2}F0,1,1,1F_{0,1,1,1}F1,0,0,2F_{1,0,0,2}F2,3F_{2,3}F0,3′′F_{0,3}^{\prime\prime}F0,1,2,0F_{0,1,2,0}F0,1,0,1F_{0,1,0,1}F1,0,1,1F_{1,0,1,1}F0,0,0,2F_{0,0,0,2}F1,3F_{1,3}F2,2F_{2,2}F2,3F_{2,3}^{\prime}F1,2′′F_{1,2}^{\prime\prime}F0,1,1,0F_{0,1,1,0}F1,0,2,0F_{1,0,2,0}F1,0,0,1F_{1,0,0,1}F0,0,1,1F_{0,0,1,1}F0,3F_{0,3}F1,2F_{1,2}F2,1F_{2,1}F2,1′′F_{2,1}^{\prime\prime}F0,2′′F_{0,2}^{\prime\prime}F1,3F_{1,3}^{\prime}F3F_{3}^{\prime}F2′′F_{2}^{\prime\prime}F0,1,0,0F_{0,1,0,0}F1,0,1,0F_{1,0,1,0}F0,0,2,0F_{0,0,2,0}F0,0,0,1F_{0,0,0,1}F0,2F_{0,2}F2,0F_{2,0}F0,3F_{0,3}^{\prime}F1,1F_{1,1}F1,1′′F_{1,1}^{\prime\prime}F2F_{2}^{\prime}F1′′F_{1}^{\prime\prime}F1,0,0,0F_{1,0,0,0}F0,0,1,0F_{0,0,1,0}F1,0F_{1,0}F0,1F_{0,1}F0,1′′F_{0,1}^{\prime\prime}F1F_{1}^{\prime}F0′′F_{0}^{\prime\prime}F0,0,0,0F_{0,0,0,0}F0,0F_{0,0}F0F_{0}^{\prime}Rank 8Rank 7Rank 6Rank 5Rank 4Rank 3Rank 2

Appendix B Details for E8E_{8} and p=2p=2

This section complements the results in Section 6.8.

B.1. The families of subgroups in [41]

Yu [41, §8] classified all elementary abelian 22-subgroups of GG, separating these into six disjoint families depending on some parameters, as follows:

  • (1)

    Fr,sF_{r,s} (r2;s3)(r\leq 2;s\leq 3). Such a subgroup has rank r+s+3r+s+3. From [41, Proposition 8.8], these have distribution 2AxBy2{\rm A}_{x}{\rm B}_{y} where x=2r+s+62rx=2^{r+s}+6\cdot 2^{r} and y=72r+s62r1y=7\cdot 2^{r+s}-6\cdot 2^{r}-1. Since there is no toral subgroup with distribution 2A72{\rm A}_{7}, we conclude that F0,0F_{0,0} is non-toral, hence all these subgroups are non-toral as they all contain F0,0F_{0,0}.

  • (2)

    Fr,sF_{r,s}^{\prime} (r,s2)(r,s\leq 2). Such a subgroup has rank r+s+2r+s+2. Its distribution is given by [41, Proposition 8.8]. The subgroup F2,2F_{2,2}^{\prime} turns out to be the unique subgroup with distribution 2A24B392{\rm A}_{24}{\rm B}_{39}, which matches a toral subgroup returned by our algorithm. Thus, F2,2F_{2,2}^{\prime} and all its subgroup Fr,sF_{r,s}^{\prime} are toral.

  • (3)

    Fϵ,δ,r,sF_{\epsilon,\delta,r,s} (ϵ+δ1;r+s2)(\epsilon+\delta\leq 1;r+s\leq 2). Such a subgroup has rank ϵ+r+2(δ+s)+3\epsilon+r+2(\delta+s)+3. According to the discussion after [41, Definition 8.15], these subgroups have distribution 2AxBy2{\rm A}_{x}{\rm B}_{y} where x=2ϵ+r+2(δ+s)+1+(1ϵ)(1)δ2r+s+δx=2^{\epsilon+r+2(\delta+s)+1}+(1-\epsilon)(-1)^{\delta}2^{r+s+\delta} and y=32ϵ+r+2(δ+s)+1(1ϵ)(1)δ2r+s+δ1y=3\cdot 2^{\epsilon+r+2(\delta+s)+1}-(1-\epsilon)(-1)^{\delta}2^{r+s+\delta}-1. Note that this does not agree with [41, Proposition 8.8(3)], which is missing an exponent ‘22’ in a given formula. In particular, F0,0,0,0F_{0,0,0,0} has distribution 2A3B42{\rm A}_{3}{\rm B}_{4}, which it shares with no toral subgroup. Hence F0,0,0,0F_{0,0,0,0} is non-toral, as are all the subgroups Fϵ,δ,r,sF_{\epsilon,\delta,r,s}.

  • (4)

    Fϵ,δ,r,sF_{\epsilon,\delta,r,s}^{\prime} (ϵ+δ1;r+s2;1s)(\epsilon+\delta\leq 1;r+s\leq 2;1\leq s). Such a subgroup has rank ϵ+r+2(s+δ)+2\epsilon+r+2(s+\delta)+2. By [41, Proposition 8.8(4)] this has distribution 2AxBy2{\rm A}_{x}{\rm B}_{y} where x=2ϵ+r+2(δ+s)+1+(1)δ(1ϵ)2r+s+δx=2^{\epsilon+r+2(\delta+s)+1}+(-1)^{\delta}(1-\epsilon)2^{r+s+\delta} and y=2ϵ+r+2(δ+s)+1(1)δ(1ϵ)2r+s+δ1y=2^{\epsilon+r+2(\delta+s)+1}-(-1)^{\delta}(1-\epsilon)2^{r+s+\delta}-1. In particular F0,1,0,2F_{0,1,0,2}^{\prime} is the unique subgroup of rank 88 with distribution 2A120B1352{\rm A}_{120}{\rm B}_{135}, hence is toral, as are all of its subgroups Fϵ,δ,r,sF_{\epsilon,\delta,r,s}^{\prime}.

  • (5)

    FrF_{r}^{\prime} (r5)(r\leq 5). Such a subgroup has rank rr. By [22, (9.2)], the groups FrF_{r}^{\prime} with r4r\leq 4 are toral, and F5F_{5}^{\prime}, the unique 2B2{\rm B}-pure subgroup of rank 55, is non-toral.

  • (6)

    Fr,s′′F_{r,s}^{\prime\prime} (r3;s2)(r\leq 3;s\leq 2). Such a subgroup has rank r+s+1r+s+1. Its distribution follows from [41, Definition 8.15], however this contains several typographic errors so we give this description again for completeness. We have decompositions

    Fr,0′′=Ar×B,Fr,1′′=Ar×C,Fr,2′′=Ar×D,F_{r,0}^{\prime\prime}=A_{r}\times B,\quad F_{r,1}^{\prime\prime}=A_{r}\times C,\quad F_{r,2}^{\prime\prime}=A_{r}\times D,

    where ArA_{r} is a 2B2{\rm B}-pure subgroup of rank rr, BB is a 2A2{\rm A}-pure subgroup of rank 11, and CC and DD are subgroups of rank 22 and 33 respectively, each containing a unique element from class 2A2{\rm A}. Then [41, Definition 8.15] states that an element lies in class 2A2{\rm A} precisely when x22Ax_{2}\in 2{\rm A} in the decomposition x=(x1,x2)x=(x_{1},x_{2}) arising from the above. In particular Dist(Fr,s′′)=2A2rB2r(2s+11)1\operatorname{Dist}(F_{r,s}^{\prime\prime})=2{\rm A}_{\phantom{(}\!\!2^{r}}{\rm B}_{2^{r}(2^{s+1}-1)-1}. From this and from inspecting the distributions of the remaining toral subgroups, we find that Fr,s′′F_{r,s}^{\prime\prime} is toral when s{0,1}s\in\{0,1\}, and is non-toral when s=2s=2.

This gives 12+9+18+9+12+6=6612+9+18+9+12+6=66 classes of subgroups in all; the non-toral ones are listed in Table 7.

B.2. Normaliser quotients

For each elementary abelian EE as above, the quotient NG(E)/CG(E)N_{G}(E)/C_{G}(E) is determined in [41, Proposition 8.17]. Adopting the same notation for matrix groups as in the E7,adE_{7,{\text{\rm ad}}} case, the normaliser structure is as in Table 10. Here a wreath product SL3(2)2\operatorname{SL}_{3}(2)\wr 2 denotes an action on a direct sum of two copies of the natural 33-dimensional module. The group S(s;ϵ,δ)S(s;\epsilon,\delta) is the group Sp(s+ϵ+2δ;ϵ,(1ϵ)(1δ))\operatorname{Sp}(s+\epsilon+2\delta;\epsilon,(1-\epsilon)(1-\delta)) in [41, p. 259]. From the description there it is not hard to show that

S(s,ϵ,δ)\displaystyle S(s,\epsilon,\delta) ={SO2s+4+(2)(ϵ,δ)=(0,1)SO2s+3(2)(ϵ,δ)=(1,0)SO2s+2(2)(ϵ,δ)=(0,0).\displaystyle=\left\{\begin{array}[]{ll}\operatorname{SO}_{2s+4}^{+}(2)&\text{: }(\epsilon,\delta)=(0,1)\\ \operatorname{SO}_{2s+3}(2)&\text{: }(\epsilon,\delta)=(1,0)\\ \operatorname{SO}_{2s+2}^{-}(2)&\text{: }(\epsilon,\delta)=(0,0).\\ \end{array}\right.

where each group is acting in its natural orthogonal representation.

Table 10. Normaliser quotients of the non-toral 22-subgroups of the algebraic group E8E_{8}
EE NG(E)/CG(E)N_{G}(E)/C_{G}(E)
Fr,sF_{r,s} (s2)(s\leq 2) (SLr(2)𝟎SLs(2)𝟎𝟎𝟎SL3(2))\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast&\ast\\ \mathbf{0}&\operatorname{SL}_{s}(2)&\mathbf{0}\\ \mathbf{0}&\mathbf{0}&\operatorname{SL}_{3}(2)\end{pmatrix}
Fr,3F_{r,3} (SLr(2)𝟎SL3(2)2)\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast\\ \mathbf{0}&\operatorname{SL}_{3}(2)\wr 2\end{pmatrix}
Fϵ,δ,r,sF_{\epsilon,\delta,r,s} (SLr(2)r,2s+ϵ+2δ+2r𝟎S(s;ϵ,δ)2s+ϵ+2δ+2𝟎𝟎1)\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast_{r,2s+\epsilon+2\delta+2}&\ast_{r}\\ \mathbf{0}&S(s;\epsilon,\delta)&\ast_{2s+\epsilon+2\delta+2}\\ \mathbf{0}&\mathbf{0}&1\\ \end{pmatrix}
Fr,s′′F_{r,s}^{\prime\prime} (SLr(2)𝟎1𝟎𝟎SLs(2))\begin{pmatrix}\operatorname{SL}_{r}(2)&\ast&\ast\\ \mathbf{0}&1&\ast\\ \mathbf{0}&\mathbf{0}&\operatorname{SL}_{s}(2)\end{pmatrix}
FrF_{r}^{\prime} SLr(2)\operatorname{SL}_{r}(2)

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