This paper investigates the structure of geometric unipotent radicals in pseudo-reductive groups over fields, providing bounds on their nilpotency class and analyzing element orders in specific cases.
Contribution
It establishes bounds on the nilpotency class of unipotent radicals in pseudo-reductive groups and examines element orders in Weil restrictions over inseparable field extensions.
Findings
01
Bounds on nilpotency class are sharp in many cases.
02
Results on element orders in unipotent radicals of Weil restrictions.
03
Structural insights into unipotent radicals of pseudo-reductive groups.
Abstract
We establish some results on the structure of the geometric unipotent radicals of pseudo-reductive k-groups. In particular, our main theorem gives bounds on the nilpotency class of geometric unipotent radicals of standard pseudo-reductive groups, which are sharp in many cases. A major part of the proof rests upon consideration of the following situation: let k' be a purely inseparable field extension of k of degree p^e and let G denote the Weil restriction of scalars R_{k'/k}(G') of a reductive k'-group G'. When G= \R_{k'/k}(G') we also provide some results on the orders of elements of the unipotent radical \RR_u(G_{\bar k}) of the extension of scalars of G to the algebraic closure \bar k of k.
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Full text
On unipotent radicals of pseudo-reductive groups
Michael Bate
Department of Mathematics,
University of York,
York YO10 5DD,
United Kingdom
We establish some results on the structure of the geometric unipotent radicals of pseudo-reductive k-groups. In particular, our main theorem gives bounds on the nilpotency class of geometric unipotent radicals of standard pseudo-reductive groups, which are sharp in many cases.
A major part of the proof rests upon consideration of the following situation: let k′ be a purely inseparable field extension of k of degree pe and let G denote the Weil restriction of scalars Rk′/k(G′) of a reductive k′-group G′. When G=Rk′/k(G′) we also provide some results on the orders of elements of the unipotent radical Ru(Gkˉ) of the extension of scalars of G to the algebraic closure kˉ of k.
2010 Mathematics Subject Classification:
20G15
1. Introduction
Let G be a smooth affine algebraic k-group over an arbitrary field k. Then G is said to be pseudo-reductive if G is connected and the largest k-defined connected smooth normal unipotent subgroup Ru,k(G) of G is trivial. J. Tits introduced pseudo-reductive groups to the literature some time ago in a series of courses at the Collège de France ([Tit92] and [Tit93]), but they have resurfaced rather dramatically in recent years thanks to the monograph [CGP15], many of whose results were used in B. Conrad’s proof of the finiteness of the Tate–Shafarevich sets and Tamagawa numbers of arbitrary linear algebraic groups over global function fields [Con12, Thm. 1.3.3]. The main result of that monograph is [CGP15, Thm. 5.1.1] which says that unless one is in some special situation over a field of characteristic 2 or 3, then any pseudo-reductive group is standard. This means it arises after a process of modification of a Cartan subgroup of a certain Weil restriction of scalars of a given reductive group (we assume reductive groups are connected). More specifically, a standard pseudo-reductive group G can be expressed as a quotient group of the form
[TABLE]
corresponding to a 4-tuple (G′,k′/k,T′,C), where k′ is a non-zero finite reduced k-algebra, G′ is a k′-group with reductive fibres over Speck′, T′ is a maximal k′-torus of G′ and C is a commutative pseudo-reductive k-group occurring in a factorisation
[TABLE]
of the natural map ϖ:Rk′/k(T′)→Rk′/k(T′/ZG′).
Here ZG′ is the (scheme-theoretic) centre of G′111Note that ϖ is not surjective when ZG′ has non-étale fibre at a factor field ki′ of k′ that is not separable over k. and C acts on Rk′/k(G′) via ψ followed by the functor Rk′/k applied to the conjugation action of T′/ZG′ on G′; we regard Rk′/k(T′) as a central subgroup of Rk′/k(G′)⋊C via the map h↦(i(h)−1,ϕ(h)), where i is the natural inclusion of Rk′/k(T′) in Rk′/k(G′) .
The structure of general connected linear algebraic groups over perfect fields k is well-understood: the geometric unipotent radical Ru(Gkˉ)=Ru,kˉ(Gkˉ) descends to a subgroup Ru(G) of G, and the quotient Gred:=G/Ru(G) is reductive. If one further insists k be separably closed one even has that Gred is split, so Gred is the central product of its semisimple derived group D(G) and a central torus, with Gred/ZG semisimple—in fact, the direct product of its simple factors.
Most of this theory goes wrong over imperfect fields k, hence in particular the need to consider pseudo-reductive groups, whose geometric unipotent radicals may not be defined over k. In order to understand the structure of a given smooth affine algebraic group G over k it is therefore instructive to extend scalars to the (perfect) algebraically closed field kˉ and analyse the structure of Gkˉ, where, for example, one sees the full unipotent radical. We pursue this approach in this paper and discuss the structure of Gkˉ where G is a standard pseudo-reductive group arising from a 4-tuple (G′,k′/k,T′,C). The reductive part Gkˉred=Gkˉ/Ru(Gkˉ) is not especially interesting in that the universal property of Weil restriction implies that Gkˉred has the same root system as G′. Further results [CGP15, Thm. 3.4.6, Cor. A.5.16] even furnish us, under some restrictive conditions, with a Levi subgroup for G: a smooth subgroup H such that Hkˉ is a complement to the geometric unipotent radical Ru(Gkˉ). However, the precise structure of Ru(Gkˉ) is rather more mysterious. While one knows that there is a composition series of Ru(Gkˉ) whose composition factors are related to the adjoint Gkˉ′-module g′=Lie(Gkˉ′) (see Lemma 3.1), it is unclear what the structure of Ru(Gkˉ) is qua group. Since Ru(Gkˉ) is a p-group, one may consider some standard invariants, which measure the order of its elements and the extent to which it is non-abelian. One major purpose of this paper is to show that as soon as the root system associated to G is non-trivial and k′/k is finite and inseparable, then Ru(Gkˉ) is almost always non-abelian (in a way that depends on the characteristic of the field amongst other things).
To state our results, let (G′,k′/k,T′,C) be a 4-tuple giving rise to a pseudo-reductive group G and denote the separable closure of k by ks. Then ks′=k′⊗kks is a finite non-zero reduced ks-algebra, isomorphic to a product of factor fields ∏iki, where each ki/ks is a purely inseparable extension. Let Gi′ (resp., Ti) denote the fibre of Gks′′ (resp., Tks′) over ki. By standard results, Rk′/k(G′)ks≅Rks′/ks(G′) (see Lemma 2.1).
If
[TABLE]
for S′ a torus and r>0, we say Gi′ is unusual. We define a number ℓi depending on Gi′ and ki. First, if Gi′ is commutative, then set ℓi=1. Now, for each field ki, form the ks-algebra Bi=ki⊗kski. Each Bi is a local ki-algebra, which by virtue of the pure inseparability of ki/ks means that its maximal ideal, mi say, consists of nilpotent elements. Hence there is a minimal n such that min=0; in case Gi′ is not unusual, let ℓi:=n−1. In case Gi′ is unusual, then define ℓi to be the minimal n such that
(2mi)n−1⋅mi2=0
where (2mi) is the ideal of squares in mi. Finally define the integer
[TABLE]
Theorem 1.1**.**
Let G be a non-commutative standard pseudo-reductive group over a field k of characteristic p, arising from a 4-tuple (G′,k′/k,T′,C) with k′ a non-zero finite reduced k-algebra. Let the Gi′ (resp., the Ti′) be the fibres of G′ (resp., T′) over the factor fields of ks, as above. Suppose that for every unusual fibre Gi′, the map ϕ in the factorisation (∗) is an injection on restriction to Ti′∩Gi′. Then the nilpotency class of Ru(Gkˉ) is N.
What the theorem indicates is that the precise structure of Ru(Gkˉ), including its nilpotency class, appears to depend in a very particular way on the nature of the extension k′/k used in Weil restriction, rather than on, for instance, the reductive group G′ (provided the reductive group contains at least one fibre that is not unusual or commutative).
Remarks 1.2*.*
(i) There is one set of cases we have excluded. After passing to an appropriate direct factor of a fibre of G′ over k′, this happens when G arises from a 4-tuple (G′,k′/k,T′,C), where G′=SL2. The kernel of the map Rk′/k(T′)→Rk′/k(T′/ZG′) is Rk′/k(μ2) (see [CGP15, Prop. 1.3.4]). For example, let us suppose in the factorisation Rk′/k(T′)→ϕC→ψRk′/k(T′/ZG′) that ker(ϕ)=Rk′/k(μ2) and ψ is injective. Then we may regard C as a subgroup of Rk′/k(T′/ZG′) sitting in between Rk′/k(T′)/Rk′/k(μ2) and Rk′/k(T′/ZG′). If C=Rk′/k(T′)/Rk′/k(μ2) then G≅Rk′/k(SL2)/Rk′/k(μ2), and the nilpotency class of the unipotent radical of Gkˉ is at most the minimal n such that (2mi)n−1⋅mi2=0 (see Remark 3.8)—in other words it is bounded above by the nilpotency class of the unipotent radical of Rk′/k(SL2)kˉ. If C=Rk′/k(T′/ZG′) then G≅Rk′/k(PGL2) (cf. Remark 3.17), so the unipotent radical of Gkˉ has nilpotency class n−1 for the minimal n such that mn=0. These numbers are usually different. In between these two extremes there is a range of possibilities: there may be many subgroups C sitting in between Rk′/k(SL2)/Rk′/k(μ2) and Rk′/k(T′/ZG′)—note that the quotient Rk′/k(T′/ZG′)/(Rk′/k(SL2)/Rk′/k(μ2)) is a smooth commutative unipotent group—and we have, a priori, no control over these.
(ii) Given any standard pseudo-reductive group G, by [CGP15, Thm. 4.1.1],
we may find a standard presentation for it; that is, a 4-tuple (G′,k′/k,T′,C) giving rise to G through the standard construction such that G′ has absolutely simple, simply-connected fibres over Speck′. In this case, one may simplify the statement of the theorem somewhat, since then a fibre of Gi′ of G′ is unusual precisely when (Gi′)ks≅SL2 and p=2.
To prove the theorem, we reduce to the case that G is a Weil restriction, but in order to deal with cases where the centre ZG′ of G′ is not smooth, we show how to present G through the standard construction, starting from a central extension G′ of G′ such that the centre of G′ is smooth (see Section 3.5). This may be of independent interest.
In Section 4 we consider for G of the form Rk′/k(G′) another invariant of Ru(Gkˉ) usually attached to p-groups—the exponent, i.e., the minimal integer s such that the ps-power map on Ru(Gkˉ) factors through the trivial group. For this invariant, we do not have as precise a result as we do for the nilpotency class, but we establish some upper and lower bounds, and identify a possible form of a precise result, cf. Question 4.6.
Finally, let us remark that part of the proof of Theorem 1.1 reduces to some bare-hands calculations with matrices arising from the Weil restriction Rk′/k(GL2) and may be of interest to anyone who would like to see some examples of pseudo-reductive groups in an explicit description by matrices.
2. Notation and Preliminaries
We follow the notation of [CGP15]. In particular, k is always a field of characteristic p>0. All algebraic groups are assumed to be affine and of finite type over the ground ring, and all subgroups are closed. Reductive and pseudo-reductive groups are assumed to be smooth and connected.
Let us recall the definition of Weil restriction and some relevant features. We consider algebraic groups scheme-theoretically, so that an algebraic k-group G is a functor {k-algebras→groups} which is representable via a finitely-presented k-algebra k[G]. Let k′ be a non-zero finite reduced k-algebra. Then for any smooth k′-group G′ with connected fibres over Speck′, the Weil restriction G=Rk′/k(G′) is a smooth connected k-group of dimension [k′:k]dimG′, characterised by the property G(A)=G′(k′⊗kA) functorially in k-algebras A. If H′ is a subgroup of G′ then Rk′/k(H′) is a subgroup of Rk′/k(G′). For a thorough treatment of this, one may see [CGP15, A.5]. Important for us is the fact that Weil restriction is right adjoint to base change: that is, we have a bijection
[TABLE]
natural in the k-group scheme M. We need two special cases. First, if M=G=Rk′/k(G′) then the identity morphism G→G corresponds to a map qG′:Gk′→G′. When k′ is a finite purely inseparable field extension of k and G′ is reductive then by [CGP15, Thm. 1.6.2], qG′ is smooth and surjective, kerqG′ coincides with Ru,k′(Gk′) and Ru,k′(Gk′) is a descent of Ru(Gkˉ) (so Ru(Gkˉ) is defined over k′); it follows from the naturality of the maps concerned that if H′ is a connected reductive subgroup of G′ then kerqH′⊆kerqG′, so Ru,k′(Hk′)⊆Ru,k′(Gk′). In particular, dimRu,k′(Gk′)=([k′:k]−1)dimG′. Second, if H is a reductive k-group and M=G′=Hk′ then the identity morphism Hk′→Hk′ corresponds to a map iH:H→Rk′/k(Hk′). When k′ is a finite purely inseparable field extension of k then by [CGP15, Cor. A.5.16], the composition Hk′⟶(iH)k′Rk′/k(Hk′)⟶qHk′Hk′ is the identity, so we may regard H as a subgroup of Rk′/k(Hk′) via iH; in fact, H is a Levi subgroup of Rk′/k(Hk′).
Let k′=∏i=1nki be a non-zero finite reduced k-algebra with factor fields ki.
Then any algebraic k′-group G′ decomposes as a product G′=∏i=1nGi′
where each Gi′ is an algebraic ki-group (it is the fibre of G′ over Specki).
In such a situation, we let Ru,k′(G′) denote the unipotent subgroup ∏i=1nRu,ki(Gi).
We have Rk′/k(G′)=∏i=1nRki/k(Gi′); in particular, Ru,k′(Rk′/k(G′)k′)=∏i=1nRu,k′(Rki/k(Gi′)k′. This allows us to reduce immediately to the case that k′ is a field in the proof of Theorem 1.1.
Suppose now that H is a smooth connected algebraic group over k and let [g,h]=ghg−1h−1 denote the commutator of the elements g,h∈H(kˉ). Let M,K be smooth connected subgroups of H. Then the commutator subgroup [M,K] is a smooth connected subgroup of H, and we may identify [M,K](kˉ) with the commutator subgroup [M(kˉ),K(kˉ)]. Moreover, [Mk′,Kk′]=([M,K])k′ for any field extension k′/k (cf. [Bor91, I.2.4]). In particular, we may form the lower central series {Dm(H)}m≥0 in the usual way, and Dm(H)(kˉ) is the mth term in the lower central series for the abstract group H(kˉ). We say that H is nilpotent if there exists some integer m such that Dm(H)=1. The nilpotency classcl(H) of H is the smallest integer m such that Dm(H)=1. The arguments above show that extending the base field does not change the nilpotency class of H.
In proving Theorem 1.1 and intermediate results, we usually want to reduce to the case that k is separably closed, guaranteeing that ki/k is purely inseparable for ki a factor field of k′. This also allows us to assume that the group G′ has split reductive fibres.
We denote by ks the separable closure of k in its algebraic closure kˉ, and we set ks′=k′⊗kks, a non-zero finite reduced ks-algebra. Note that even when k′ is a field, ks′ need not be a field.
Lemma 2.1**.**
Let G be a standard pseudo-reductive group arising from (G′,k′/k,T′,C). Then
(i) Gks is isomorphic to the standard pseudo-reductive group arising from (Gks′′,ks′/ks,Tks′′,Cks).
(ii) Ru,k′(Gk′)ks′=Ru,ks′(Gks′).
Proof.
(i). We have G=(Rk′/k(G′)⋊C)/Rk′/k(T′). In order to see that
[TABLE]
it suffices to see that: (a) the sequences
[TABLE]
and
[TABLE]
remain exact after taking the base change to ks, with the second remaining split; and (b) the formation of the Weil restriction Rk′/k(G′) commutes with base change to ks.
These facts are standard: for (a) this follows since algebras over a field k are flat; and (b) is [CGP15, A.5.2(1)].
(ii). Without loss we can assume k′ is a field. Write ks′=∏i∈Iki. Since
[TABLE]
we have Ru,k′(Gk′)ki=Ru,ki(Gki) for each i∈I. The result now follows.
∎
The following result provides an upper bound for the nilpotency class of Ru(Rk′/k(G′)kˉ) in case k′ is a purely inseparable field extension. We will later reduce to this case.
Proposition 3.1**.**
Let G=Rk′/k(G′) for k′ a purely inseparable field extension of k. Then B:=k′⊗kk′ is local with maximal nilpotent ideal m. Suppose n is minimal such that mn=0. Then Ru(Gkˉ) has a filtration Ru(Gkˉ)=U1⊇U2⊇⋯⊇Un=1 satisfying the following:
(a) the successive quotients are Gkˉ′-equivariantly isomorphic to a direct sum of copies of the adjoint Gkˉ′-module;
(b) the commutator subgroup [U1,Ui]⊆Ui+1 for any i≥1. In particular, we have cl(Ru(Gkˉ))≤n−1.
Proof.
Following [Oes84, A.3.6], we can identify Gk′=Rk′/k(G′)k′ with
RB/k′(GB′) where B:=k′⊗kk′.
For the convenience of the reader, we reproduce some of the constructions from [Oes84, §A.3.5] in this setting.
We begin with some basic observations and notation.
The maximal ideal m of B is the kernel of the map B→k′ which sends b1⊗b2→b1b2,
so m is generated by elements of the form b⊗1−1⊗b.
This is an ideal of nilpotent elements (everything is killed by a suitably high power of p),
so there is n∈N
such that mn={0}; choose n minimal subject to this.
Note that n≤[k′:k] since B has dimension [k′:k] as a (left) vector space over k′,
so this is the largest possible size for a strictly decreasing chain of proper subspaces of B.
Denote the quotient B/mi for 1≤i≤n by Bi and let Gi:=RBi/k′(GBi′).
Note that since B1=B/m≅k′ we have that G1≅G′ and since mn={0} we have that
Gn≅Gk′.
It is proved in [Oes84, Prop. A.3.5] that the canonical surjection Bi→Bi−1 for each 1≤i≤n gives rise to a surjective homomorphism of algebraic groups
Gi→Gi−1; let Vi denote the kernel of this map for each i.
Let A:=k′[G′]⊗k′B denote the coordinate algebra of GB′,
and let Ai:=k′[G′]⊗k′Bi denote the coordinate algebra of GBi′ for each i
(recall that An=A).
In [Oes84, Prop. A.3.5], Oesterlé observes that each Vi is a vector group naturally isomorphic to the additive group Lie(G′)⊗k′mi−1/mi.
We recall how to see this.
Given any k′-algebra R,
the identity element of Gi(k′) gives a homomorphism of Bi-algebras Ai→Bi which we can compose with the canonical injection Bi→R⊗k′Bi to get a homomorphism ei:Ai→R⊗k′Bi.
Then one notes that an R-point v∈Vi(R) corresponds to a
Bi-algebra homomorphism v:Ai→R⊗k′Bi whose difference with ei has image in
R⊗k′mi−1/mi.
The ring R⊗k′mi−1/mi is also an Ai-module via the identity element of Gi(k′):
multiplication by an element a∈Ai under this action coincides with multiplication by ei(a)
in R⊗k′mi−1/mi.
Now, given a,b∈Ai, we write
[TABLE]
The last term above is a product of terms in R⊗k′mi−1/mi, so is zero,
and hence we can conclude that ei−v acts like a Bi-linear derivation δ:Ai→R⊗k′mi−1/mi (with the Ai-module structure we have given).
Conversely, any such derivation will gives rise to an element of Vi(R) by reversing the above process.
Any Bi-linear derivation of Ai in R⊗mi−1/mi will kill the ideal (m/mi)Ai in Ai (since it is Bi-linear and multiplication by m/mi in R⊗k′mi−1/mi kills everything); this means we can identify this set of derivations with the k′-linear derivations of Ai/(m/mi)Ai≅k′[G′] in R⊗mi−1/mi—write Derk′(k′[G′],R⊗k′mi−1/mi) for this set.
Further, since the Ai-module structure on R⊗mi−1/mi comes from the identity element in Gi(R)=G′(R⊗Bi), we see that the induced k′[G′]-module structure
permits an identification
[TABLE]
Now the set of derivations on the right hand side is just Lie(G′),
so we have the required identification of Vi(R) with Lie(G′)⊗k′R⊗k′mi−1/mi.
We now show the identifications in the previous paragraphs turn group multiplication in Vi(R) into addition.
Given v1,v2∈Vi, the idea is to rewrite
[TABLE]
and then
to note that when we apply this equation to a∈Ai the final term is zero in R⊗mi−1/mi.
To justify this, given a∈Ai let ∑r,sar⊗as denote the image of a under the comultiplication map Ai→Ai⊗Ai.
Then recalling that ei comes from the identity of Gi(k′), we can write:
[TABLE]
where the third sum on the penultimate line is zero in R⊗mi−1/mi, being a sum of products.
So we see that each successive quotient Vi is a vector group as claimed.
We now recall that there is a natural copy of G′ inside Gi –
on the level of R-points for a k′-algebra R, this comes from the observation that
any k′-algebra homomorphism k′[G′]→R has a canonical
extension to a Bi-algebra homomorphism Ai=k′[G′]⊗Bi→R⊗Bi.
This copy of G′ acts on Vi by conjugation, and the replacement of v∈Vi(R) with
ei−v is clearly equivariant with respect to this action.
On the other hand, under the identification of Lie(G′) with Derk′(k′[G′],k′), the adjoint action comes from the action of G′ on k′[G′] induced by the conjugation action of G′ on itself.
This in turn, gives rise to the action of Gi on Ai=k′[G′]⊗Bi induced by conjugation after Weil restriction, and the canonical copy of G′ acts via its action on the first factor in this tensor product.
Hence we see that the isomorphism of vector groups we have established above is G′-equivariant.
Now this is established, we show how to piece together the Vi to give the claims in the proposition. Since the natural map B=Bn→Bi for each 1≤i≤n is the composition of the natural maps Bn→Bn−1→⋯→Bi, we also have surjective maps Gk′≅Gn→Gi;
let Ui denote the kernel of this map for each i.
Then U1 is the geometric unipotent radical of G and U1⊃U2⊃⋯⊃Un.
We also see that Ui/Ui+1≅Vi+1 for each 1≤i≤n−1.
So we have a filtration of the unipotent radical with successive quotients equal to the groups Vi.
The final step is to check that the commutator [U1,Ui]⊆Ui+1 for each i,
so that this filtration is compatible with the lower central series for U1.
For this, given a k′-algebra R, let u∈U1(R) and v∈Ui(R)
and as usual identify u and v with B-algebra homomorphisms A→R⊗B.
Analogously with above, we want to rewrite the commutator in a nice way.
Recall that in this set-up we have denoted by ei the homomorphisms Ai→R⊗Bi coming from the identity of Gi(k′).
To ease notation, denote en=e.
Note that for each i, ei coincides with e modulo mi, and the homomorphisms e, u
and v have the same domain and codomain.
Then one equation to use (of the many possible) is
[TABLE]
Apply this to a∈A.
Note that since u∈U1, (e−u)(a)∈R⊗k′m.
Similarly, since v∈Ui, (e−v)∈R⊗k′mi modulo mi+1.
Therefore the second term on the right-hand side is zero modulo mi+1.
Similarly the first term is zero, noting that vu−1v−1∈U1.
Therefore, the whole right-hand side, and hence the left-hand side, is zero in Ui/Ui+1, which is what we wanted.
Again, this calculation can be justified using the comultiplication.
∎
When G′ is not unusual—that is, it is non-commutative and either p=2 or G′ is not a direct product of some copies of SL2 with a torus—then we show in the next sections that the upper bound for cl(Ru(Gkˉ)) in the proposition above is in fact also a lower bound.
Example 3.2**.**
Note that the filtration from Proposition 3.1 need not exist for an arbitrary standard pseudo-reductive group. For example, if p=2, G′=SL2, k′/k is a purely inseparable field extension of degree 2 and G is the standard pseudo-reductive group Rk′/k(G′)/Rk′/k(μ2), then G has dimension dimG′⋅[k′:k]−(p−1)=5; see [CGP15, Ex. 1.3.2]. Since G′=SL2 is defined over k, there is a canonical copy of G′ inside Rk′/k(G′)k′. Factoring out by Rk′/k(μ2)k′ kills the copy of μ2 inside G′, so we obtain a copy of PGL2 inside Gk′. This gives rise to a copy of Lie(PGL2) in Lie(Gk′), so we see that Lie(Ru(Gkˉ)) cannot be a sum of copies of Lie(G′)kˉ, just for dimensional reasons. (Similar examples can be given for any G′ whose centre is not smooth.)
3.2. Lower bound
Let k′/k be a purely inseparable field extension, and set B=k′⊗kk′ with maximal ideal m. In this section we do a calculation in GL2(B) which shows that Ru(Rk′/k(GL2)kˉ) has nilpotency class exactly n−1, where n is minimal such that mn=0. (Of course the upper bound has already been established in the previous section.)
Let G=Rk′/k(GL2). It suffices to compute the nilpotency class of Ru,k′(Gk′) since this is a k′-form of the geometric unipotent radical. As in the proof of Proposition 3.1 we have Rk′/k(GL2)k′=RB/k(GL2), and the k′-radical of this is the kernel of the map induced from B→k′ with kernel m. Thus the k′-points of Ru,k′(Gk′) are simply the matrices
[TABLE]
By minimality of n, we can find m∈m and mi∈m for 1≤i≤n−2 such that m⋅m1⋯mn−2=0. Certainly it suffices to find the desired lower bound for cl(Ru(Gkˉ)) on the level of the k′-points of Ru,k′(Gk′), so it suffices to see that there exist z,y1,…,yn−2∈Ru,k′(Gk′)(k′) with [y1,[y2,[…,[yn−2,z]]]]=1. In the light of that observation, take
[TABLE]
then an elementary calculation yields
[TABLE]
Combining with the lower bound from Prop. 3.1, we have proved
Lemma 3.3**.**
Let k′/k be a purely inseparable field extension.
Then
[TABLE]
where n is minimal such that mn=0.
We wish to deduce the analogous result for PGL2 and SL2 (the latter when p=2). To do this we need the following two lemmas, which we also use in the proof of Theorem 1.1.
Lemma 3.4**.**
Let k′/k be a finite field extension and let G′ be a semisimple k′-group such that Z′:=ZG′ is smooth. Let Gad′=G′/Z′ and let G:=Rk′/k(G′). Then there is a natural isomorphism
[TABLE]
Proof.
Since Z′ is smooth, there is a smooth isogeny giving rise to the exact sequence
[TABLE]
By [CGP15, A.5.4(3)], Weil restriction preserves the exactness of this sequence, and so there is an exact sequence
[TABLE]
This gives, after base change to k′, an exact sequence
[TABLE]
Now Z′ is a smooth finite group scheme, so Z′≅Rk′/k(Z′)k′ as algebraic groups. This implies that Rk′/k(π)k′ is a smooth isogeny. It follows that the map Rk′/k(π)kˉ:Gkˉ→Rk′/k(Gad′)kˉ obtained by base change to kˉ gives rise to an isomorphism from Ru(Gkˉ) to Ru(Rk′/k(Gad′)kˉ). But Ru(Gkˉ) and Ru(Rk′/k(Gad′)kˉ) are defined over k′, so Rk′/k(π)k′ gives an isomorphism from Ru,k′(Gk′) to Ru,k′(Rk′/k(Gad′)k′), as required.
∎
Lemma 3.5**.**
Let k′,k,G′,Z′ and Gad′ be as in Lemma 3.4, but without the assumption that Z′ is smooth. Further, let C be a commutative pseudo-reductive k-group occurring in a factorisation of the map Rk′/k(T′)→Rk′/k(T′/Z′) for T′ a maximal k′-torus of G′. Then:
(i) We have
[TABLE]
(ii) If moreover Z′ is smooth, we have
[TABLE]
where in the final term we quotient by the usual central copy of Rk′/k(T′) occurring in the standard construction.
Proof.
(i) Let H:=(Rk′/k(G′)⋊C)kˉ and G:=((Rk′/k(G′)⋊C)/Rk′/k(T′))kˉ. We have an epimorphism f:H→G. Let U=Ru(H). Then U′:=f(U) is a smooth, connected normal unipotent subgroup of G, and so we get an epimorphism from the reductive group H/U onto G/U′. But H/U is reductive, so G/U′ must be reductive. This means U′ contains (and therefore equals) Ru(G). Thus U′ is a quotient of U and so cl(U′)≤cl(U), proving the inequality.
For the equality, we have trivially cl(U)≥cl(Ru,k′(Rk′/k(G′)k′)), so we will be done if we can show D(U)⊆D(Ru(Rk′/k(G′)kˉ)). Now C factorises the map Rk′/k(T′)→Rk′/k(T′/Z′), whose kernel is Rk′/k(Z′) (due to left exactness of Weil restriction). If A is any k-algebra and g∈C(A) then for any q∈Rk′/k(G′)(A) we can find h∈Rk′/k(T′)(A) such that hqh−1=gqg−1. In particular, [Ru,k′(Rk′/k(G′))k′,Ck′]⊆[Ru,k′(Rk′/k(G′))k′,Ru,k′(Rk′/k(G′))k′] as required.
(ii)
Let ϕ:Rk′/k(T′)→C be the map in the factorisation. Set Z=Rk′/k(Z′). Thanks to the isomorphism of groups Z′≅Zk′ arising from the hypothesis on Z′, we have by the arguments of Lemma 3.4 a smooth isogeny
[TABLE]
or equivalently
[TABLE]
where we write D in place of C/ϕ(Z). The argument of Lemma 3.4 yields an isomorphism
[TABLE]
The map C→Rk′/k(T′/Z′) gives rise to a map κ:D→Rk′/k(Gad′). We claim that the map τ:Rk′/k(Gad′)⋊D→Rk′/k(Gad′)×D given on the level of A-points by (g,d)↦(gκ(d),d) is an isomorphism. To see this, first recall (g,d)(h,e)=(gκ(d)hκ(d)−1,de). Then (g,d)(h,e)↦(gκ(d)hκ(d)−1κ(de),de)=(gκ(d)hκ(e),de) which is the product of (gκ(d),d) and (hκ(e),e) in the direct product as required.
With this in mind, we get
[TABLE]
but the commutativity of D implies that cl(Ru,k′((Rk′/k(Gad′)⋊D))k′)=cl(Ru,k′(Rk′/k(Gad′)k′)). This proves the first equality of the lemma.
To see the second equality, observe that Rk′/k(T′/Z′)≅Rk′/k(T′)/Z since Z′ is smooth. We see that the map (Rk′/k(G′)⋊C)k′→(Rk′/k(Gad′)⋊D)k′ from (∗) takes the copy of Rk′/k(T′)k′ onto the copy of Rk′/k(T′/Z′)k′, so the induced map of quotient groups yields an isogeny
[TABLE]
for some N. This isogeny is smooth because the canonical projections to the quotient groups are smooth. By the argument of Lemma 3.4 again, we get an isomorphism
[TABLE]
Now ϕk′ induces a map Φ from Rk′/k(T′/Z′)k′ onto a smooth subgroup of D, and it is easily checked that τ gives rise to an isomorphism
[TABLE]
The commutativity of D again gives the result.
∎
We can now tackle
Proposition 3.6**.**
Suppose k′/k is a purely inseparable field extension and G=Rk′/k(G′), where G′ is one of GL2 or PGL2 or SL2 (the final case only if chark=2). Let n be minimal such that mn=0. Then cl(Ru(Gkˉ))=n−1.
Proof.
In the cases considered ZG′ is smooth, so by Lemmas 3.4 and 3.5 the nilpotency classes of Ru,k′(Rk′/k(GL2)k′), Ru,k′(Rk′/k(PGL2)k′) and Ru,k′(Rk′/k(SL2)k′) are all equal. But Lemma 3.3 now supplies the result.
∎
3.3. SL2 in characteristic 2
In this section we wish to study the case G′=SL2 and G=Rk′/k(G′), where chark=2 and k′/k is a purely inseparable field extension.
We will show
Lemma 3.7**.**
Let k′/k be a purely inseparable finite field extension and let B=k′⊗kk′, with maximal ideal m. Furthermore, denote by 2m the ideal generated by the squares of the elements in m. Suppose n is the minimum such that (2m)n−1⋅m2=0. Then cl(Ru(Gkˉ))=n.
Proof.
By Lemma 2.1 we may assume k=ks. We use arguments analogous to those in the previous section.
First we establish the upper bound.
Recall that we have R:=Ru,k′(Gk′)=kerφ where φ:Gk′→G′ is the map induced by reduction modulo m. Since we will be working with commutator subgroups it is convenient to work with the kˉ-points of R. Set B=B⊗k′kˉ=k′⊗kkˉ and m=m⊗k′kˉ. Then B is local with unique maximal ideal m and quotient field kˉ. The ideal m is nilpotent and the minimal n with mn=0 is the same as the minimal n with mn=0.
Define ideals Ir and Jr of B for r≥0 by I0=J0=m, Ir=(2m)r⋅m for r≥1 and Jr=(2m)r−1⋅m2 for r≥1. Set Iˉr=Ir⊗k′kˉ=(2m)r⋅m and Jˉr=Jr⊗k′kˉ=(2m)r−1⋅m2. It is clear that Jˉr=0 (resp., Iˉr=0) if and only if Jr=0 (resp., Ir=0) for each r. Observe that Iˉr⊆Jˉr, 2m⋅Iˉr⊆Iˉr+1, 2m⋅Jˉr⊆Jˉr+1 and m⋅Iˉr⊆Jˉr+1 for all r.
Define Rr⊆G(kˉ) by
[TABLE]
It is easily checked that R0=R(kˉ) and each Rr is a subgroup of R(kˉ). Let M=(1+m1m3m21+m4)∈Rr for some given r. Consider the following matrices of R0:
[TABLE]
We have M−1=(1+m4m3m21+m1) and so we find the commutator
[TABLE]
We see that [M1,M] belongs to Rr+1. By symmetry, the commutator [M1⊤,M] also belongs to Rr+1 (here M1⊤ denotes the transpose of M1). Similarly, noting that (1+m)−1=1+m+m′ for some m′∈2m, we have
[TABLE]
which belongs to Rr+1.
These calculations together show that if n is such that Jˉn=0, then
[X1,[X2,…,[Xn,g]]]=1 for arbitrary g∈R(kˉ) and arbitrary Xi chosen from elements of the form M1, M1⊤ and M2.
Let (U′)− denote the lower root group of G′, T′ denote the diagonal torus and U′ denote the upper root group, and set U:=Rk′/k(U′), C:=Rk′/k(T′), U−:=Rk′/k((U′)−). Then the multiplication map μ:U−×C×U→G is an open immersion by [CGP15, Cor. 3.3.16].
Moreover, the intersections Rk′/k(U)kˉ∩Rkˉ, Rk′/k(T)kˉ∩Rkˉ, Rk′/k(U−)kˉ∩Rkˉ have codimension 1 in Rk′/k(U)kˉ, Rk′/k(T)kˉ, Rk′/k(U−)kˉ, respectively; this can be seen by looking at the kernel of the restriction of φkˉ to these subgroups, where φ is the map above. It follows that μkˉ(D) has codimension 3 in Rk′/k(G′)kˉ, where D:=(Rk′/k(U)kˉ∩Rkˉ)×(Rk′/k(T)kˉ∩Rkˉ)×(Rk′/k(U−)kˉ∩Rkˉ). In particular, μkˉ(D) is an open subset of Rkˉ, hence generates Rkˉ.
But, in light of the identity [x,zy]=[x,y]⋅[x,z]y and the fact from the previous paragraph that [X1,[X2,…,[Xn,R(kˉ)]]]=1 for generators Xi of R(kˉ), we are done for the upper bound.
For the lower bound, we exhibit an explicit nonzero commutator, in an analogous way to Lemma 3.3. Let n be as in the statement.
If n=1 then there is nothing to do, so suppose n>1.
Since we’re assuming that n is minimal such that Jn=0, we may pick m1,…,mn−2∈m and m,m′∈m such that m12⋯mn−22mm′ is non-zero. Take
[TABLE]
for 1≤i≤n−2. Set w=[y1,[y2,[…,[yn−2,z]]]]. Then a calculation yields
[TABLE]
and
[TABLE]
This gives the lower bound.
∎
Remark 3.8*.*
Consider the pseudo-reductive group Rk′/k(SL2)/Rk′/k(μ2). Since the canonical projection Rk′/k(SL2)→Rk′/k(SL2)/Rk′/k(μ2) is surjective on kˉ-points, Ru((Rk′/k(SL2)/Rk′/k(μ2))kˉ)(kˉ) is a quotient of Ru(Rk′/k(SL2)kˉ)(kˉ), so the nilpotency class c of the latter is at most n (where n is as in Lemma 3.7). The image of the commutator w from above in Ru((Rk′/k(SL2)/Rk′/k(μ2))kˉ)(kˉ) does not vanish, so c is at least n−1 (note that we may identify Ru(Rk′/k(μ2)kˉ)(kˉ) with the group of matrices of the form (1+m001+m) with m∈m and m2=0). The image of [z′,w], however, does vanish. It follows that c is either n or n−1; we do not know which.
Example 3.9**.**
(i). Consider the case that k′=k(t) with t2∈k∖k2.
Then m2=0, so J1=0. We can calculate:
[TABLE]
for all mi∈m.
Thus the unipotent radical is abelian in this case, so the nilpotency class is indeed 1.
(ii). Now let k′=k(s,t) of degree 4, where s2,t2∈k∖k2. We see that 2m=0 but m2=0, so J1=0 and J2=0. Choose m1=s⊗1+1⊗s∈m and m2=t⊗1+1⊗t∈m.
Note that m1m2=0, and hence if we set
[TABLE]
we have u1u2=u2u1, so the unipotent radical in this case is not abelian. In fact, we see from Lemma 3.7 that the nilpotency class is 2.
3.4. The case of Weil restrictions
We will treat here the case that G is a Weil restriction Rk′/k(G′) for G′ a reductive k′-group, where k′ is a finite reduced non-zero k-algebra. We deal with some special situations relating to the case where some fibre of G′ is unusual.
Lemma 3.10**.**
Suppose p=2. Let H′=SL2 and suppose G′=S′H′ is a split reductive group, where S′ is a central torus of G′. Then either the product map S′×H′→G′ is an isomorphism or G′ contains a copy of GL2.
Proof.
The group G′ has semisimple rank 1, so by [Mil12, Thm. 21.55], G′ is isomorphic to one of SL2×T′, GL2×T′ or PGL2×T′ for some torus T′. The result follows.
∎
Lemma 3.11**.**
Let k′ be a field and G′ a noncommutative split reductive k′-group. Then exactly one of the following holds:
(i) G′ has a subgroup isomorphic to GL2 or PGL2;
(ii) G′=(SL2)r×S′ for some r≥1.
Proof.
Suppose G′ has no subgroup isomorphic to GL2 or PGL2. If G′ contains a subgroup of type A2 then G′ contains a copy of GL2, which is impossible; note that this also implies G′ does not contain a subgroup of type G2. If G′ has a simple factor H′ of type B2 then the long-root Levi subgroup of H′ is isomorphic to GL2 if H′ is simply connected, and to Gm×PGL2 if H′ is adjoint, which gives a contradiction in both cases. So every simple factor of G′ is isomorphic to SL2.
Let H1′,…,Hr′ be the simple factors of G′ and let S′=Z(G′)0. Multiplication gives a central isogeny φ:H1′×⋯×Hr′×S′→G′.
Suppose φ is not an isomorphism. Then the projection of ker(φ) to H1′, say, must be non-trivial. Let T′ be a split maximal torus of H2′×⋯×Hr′×S′. Since ker(φ) is contained in a maximal torus of H1′×T′, we must have that φ is not injective on H1′×T′. It follows from Lemma 3.10 that H1′T′⊆G′ contains a copy of GL2.
∎
We can now prove Theorem 1.1 for the case of Weil restrictions of reductive groups. Note that such groups are of course standard pseudo-reductive, taking C=Rk′/k(T′), and ϕ an isomorphism.
By Lemma 2.1 we may assume k=ks.
Since G is a direct product of Rki/k(Gi′) for some inseparable field extensions ki/k and fibres Gi′ of G′ over k′, we will clearly have cl(Ru(Gkˉ))=maxi(Ru(Rki/k(Gi′)kˉ)). Hence it suffices to show that the nilpotency class of the unipotent radical of Gi:=Rki/k(Gi′) is the number ℓi from the introduction.
The case that Gi′ is commutative is obvious, so assume Gi′ is non-commutative. It is of course split since k=ks. If Gi′ is not unusual, then Lemma 3.11 says that Gi′ contains a copy of PGL2 or GL2. In this case Proposition 3.6 gives cl(Ru((Gi)kˉ))≥ℓi and Proposition 3.1 gives cl(Ru((Gi)kˉ))≤ℓi. Lastly, if Gi′ is unusual, then Gi is isomorphic to Rki/k(SL2)r×Rki/k(S′) for some torus S′ and some r≥1, by Lemma 3.11. Then the result follows from Lemma 3.7.
∎
3.5. Centrally smooth enlargements
The following is essentially a definition from [Mar99].
Definition 3.13**.**
Let G′ be a reductive k′-group, where k′ is a field. A centrally smooth enlargement of G′ is a reductive k′-group G′ such that Z(G′) is smooth, G′⊆G′ and G′ is generated by G′ and a central torus.
Lemma 3.14**.**
Let G′ be a split reductive k′-group. There exists a centrally smooth enlargement G′ of G′.
Proof.
This follows from [Mar99, Thm. 4.5]. The result in loc. cit. is stated only for algebraically closed fields, but the proof works for arbitrary split reductive groups, by the existence and isogeny theorems for split reductive groups [Spr98, 16.3.2, 16.3.3].
∎
Remark 3.15*.*
There is also another, simpler, proof which works for the non-split case as well: embed Z(G′) in a torus S′: for example, we could choose S′ to be a maximal torus of G′. Then set G′=(G′×S′)/N, where N is the image of Z(G′) under the obvious diagonal embedding. (Since N∩(1×S′)=1, S′ appears as a subgroup of G′.)
Let (G′,k′/k,T′,C) be a 4-tuple corresponding to a standard pseudo-reductive group
[TABLE]
with a factorisation Rk′/k(T′)→ϕC→ψRk′/k(T′/ZG′). Assume k′ is a field. Suppose G′=G′S′ is a central enlargement of G′, where S′ is a central torus of G′.
Set Z′=Z(G′), Z′=Z(G′) and T′=T′S′. It is easy to see that Z′=Z′S′⊆G′S′. Therefore the composition T′→T′→T′/Z′ induces an isomorphism β:T′/Z′→T′/Z′.
Lemma 3.16**.**
cl(Ru,k′(Gk′))≤cl(Ru,k′(Rk′/k(G′)k′)).
Proof.
The idea is to embed Rk′/k(G′)⋊C in a group of the form Rk′/k(G′)⋊C arising from a 4-tuple (G′,k′/k,T′,C) and a factorisation Rk′/k(T′)→ϕC→ψRk′/k(T′/Z′); the latter group is easier to understand than the former because Z′ is smooth. Define a homomorphism κ:Rk′/k(T′)→C×Rk′/k(T′) by κ=ϕ×ι−1, where ι:Rk′/k(T′)→Rk′/k(T′) is inversion and we identify Rk′/k(T′) naturally as a subgroup of Rk′/k(T′), say via a map iT′.
Note that κ maps Rk′/k(T′) isomorphically onto its image, which we denote by N.
Set C=(C×Rk′/k(T′))/N and let πC:C×Rk′/k(T′)→C be the canonical projection.
We claim that C is pseudo-reductive.
To see this, let V denote the preimage of Ru,k(C) in C×Rk′/k(T′).
Projection onto the second factor here maps N isomorphically onto the natural copy of Rk′/k(T′) in the second factor.
Hence if we project to the second factor and then quotient by this copy of Rk′/k(T′), the subgroup V gets mapped to a smooth unipotent k-subgroup of the commutative group Rk′/k(T′)/Rk′/k(T′).
Since this last group is a subgroup of the commutative pseudo-reductive group Rk′/k(T′/T′), it is pseudo-reductive,
and hence we conclude that the projection of V to the second factor of C×Rk′/k(T′)
is contained in the projection of N.
Hence V⊆C×Rk′/k(T′).
We have a map ψ:C×Rk′/k(T′)→C defined by ψ(c,x)=cϕ(x)−1 for c∈C(A) and x∈Rk′/k(T′)(A), where A is any k-algebra. Clearly the kernel of ψ is N, which is smooth, so ψ is smooth. Hence ψ(V) is a smooth unipotent k-subgroup of C, and is therefore trivial. It follows that V⊆N, so Ru,k(C)=1 as required.
We have obvious inclusions iC:C→C×Rk′/k(T′) and i′:Rk′/k(T′)→C×Rk′/k(T′). Define j:C→C by j=πC∘iC; then j is an embedding of C in C since N∩(C×1)=1. Now define ϕ:Rk′/k(T′)→C by ϕ=πC∘i′. It follows from the construction that j∘ϕ=ϕ∘Rk′/k(iT′).
Consider the homomorphism C×Rk′/k(T′)→Rk′/k(T′/Z′) given by the composition
[TABLE]
where the third map is multiplication and πT′:T′→T′/Z′ is the canonical projection. The kernel of this homomorphism contains N, so we get an induced homomorphism ψ:C→Rk′/k(T′/Z′). It follows from the construction that ψ∘j=Rk′/k(β)∘ψ. One can now check that the map Rk′/k(iG′)×j:Rk′/k(G′)⋊C→Rk′/k(G′)⋊C is an embedding of groups, where iG′ is the inclusion of G′ in G′.
Now G is a quotient of Rk′/k(G′)⋊C, so
[TABLE]
[TABLE]
here the equality follows from Lemma 3.5(ii) applied to (G′,k′/k,T′,C), and the final inequality holds because the canonical projection G′→G′/Z′ is smooth. This proves the result.
∎
As in the proof of Proposition 3.12 we may reduce to the case that k=ks and by passing to a fibre of G′ above k′, we may assume k′/k is a purely inseparable field extension. Certainly we are done if G′ is commutative, so assume otherwise.
If G′ is unusual, then by assumption, the map Rk′/k(T′)→C is a monomorphism.
As in the proof of Lemma 3.5 we have that the semidirect product Rk′/k(G′)⋊C is actually isomorphic to a direct product via (g,d)↦(gd,d), and so the quotient by the central subgroup N:=Rk′/k(T′)⊆Rk′/k(G′)⋊C from the standard construction gives the group Rk′/k(G′)×C′, where C′≅C/Rk′/k(T′). In particular, by Proposition 3.12 the nilpotency class of the unipotent radical is as claimed. Hence we can assume G′ is not unusual.
We get an upper bound for cl(Ru(Rk′/k(G′)kˉ)) from Lemma 3.16. Proposition 3.12 applied to G′, where G′ is a central enlargement of G′, then gives the desired upper bound.
To complete the proof, it is enough to show that cl(Ru(Rk′/k(G′)k′))≤cl(Ru(Gk′)).
By Lemma 3.11 and Proposition 3.12, G′ has a subgroup H′ isomorphic to one of SL2, GL2 or PGL2 such that
[TABLE]
Furthermore, if p=2, since G′ is not unusual, it follows that H is GL2 or PGL2. We may regard Rk′/k(H′)⊆Rk′/k(G′) as subgroups of Rk′/k(G′)⋊C in the obvious way. Let π:Rk′/k(G′)⋊C→G be the projection of the standard construction. Now ker(π) is a smooth central subgroup of Rk′/k(G′)⋊C and it follows from the definition of π that ker(π)∩Rk′/k(G′) is contained in the kernel of the map Rk′/k(T′)→Rk′/k(T′/Z′), which is Rk′/k(Z′) by [CGP15, Prop. 1.3.4]. So M:=ker(π)∩Rk′/k(H′) is a central subgroup of Rk′/k(H′). Now Rk′/k(H′)/M is a subgroup of G, so Ru((Rk′/k(H′)/M)kˉ) is a subgroup of Ru(Gkˉ). But if ZH′ denotes the centre of H′ then
[TABLE]
[TABLE]
since ZH′ is smooth, and we are done by Proposition 3.12.
∎
3.6. When k′/k is a primitive field extension.
Here we work out the consequences of Theorem 1.1 in case k′=k(t) for q=pe the order of t in k′/k. As ever, we may assume k is separably closed so that k′/k is purely inseparable. In this situation, the ideal m=⟨1⊗t−t⊗1⟩ of B is a principal ideal and it is easy to see that the minimal n such that mn=0 is just q, since (1⊗t−t⊗1)q=1⊗tq−tq⊗1=tq⊗1−tq⊗1=0. Hence the value of N in Theorem 1.1 is q−1. In particular, if G′ is not unusual or commutative, then cl(Rk′/k(G′))=q−1.
On the other hand, if G′ is unusual, then p=2 and 2m=m2. From this one readily deduces that the value of N in Theorem 1.1 is just q/2 and in particular cl(Ru(Rk′/k(G′)kˉ))=q/2.
Remark 3.17*.*
Applying the standard construction to the Weil restriction of a reductive group can change the nilpotency class of the unipotent radical; in other words, it can happen that cl(Ru(Rk′/k(G′)kˉ)) is strictly less than cl(Ru(Gkˉ)). For instance, suppose p=2 and k′/k is a primitive purely inseparable field extension of degree q≥4. Let G′=SL2, let T′ be a maximal torus of G′ and let Z′=Z(G′). Let C=Rk′/k(T′/Z′) and take the factorisation Rk′/k(T′)→C→Rk′/k(T′/Z′) to be the obvious one. Then G=(Rk′/k(G′)⋊C)/Rk′/k(T′)≅Rk′/k(PGL2), so cl(Ru(Gk′))=q−1; but cl(Ru(Rk′/k(G′)k′))=cl(Ru(Rk′/k(SL2)k′))=2q by the remarks above.
Note, however, that by Lemma 3.16—which holds for an arbitrary standard pseudo-reductive group—the nilpotency class of Ru(Gkˉ) is bounded above by n, where n is the smallest positive integer such that mn vanishes. This is the case even when k′/k is not primitive.
4. Orders of elements in unipotent radicals of Weil restrictions
In this section we collect some observations about the orders of elements in unipotent radicals Ru(Gkˉ)(kˉ),
where G=Rk′/k(G′) is the Weil restriction of a reductive group G′. More precisely, we wish to say something about the exponent e of G; that is, the minimal integer such that the pe-power map on G factors through the trivial group. Clearly e is stable under base change, so by Lemma 2.1 it suffices to consider the case where k is separably closed. Of course one could let k′ be a non-zero reduced k-algebra, but by passing to a fibre, it does no harm to assume k′/k is a purely inseparable field extension.
Since k′/k is purely inseparable, Proposition 3.1 provides a crude upper bound:
as usual, letting B=k′⊗kk′ with maximal ideal m, we have a filtration of the unipotent radical Ru(Gkˉ) with n abelian quotients, where n is the minimal positive integer such that mn=0.
Since we know each quotient is a vector group isomorphic to a direct sum of copies of the adjoint module for G′,
all elements in the quotients have order p, and we see that pn is an upper bound for the order of elements in Ru(G).
Our next result shows that we can immediately do better than this with quite an elementary argument.
Lemma 4.1**.**
With notation as above, let s be minimal such that ps≥n.
Then the exponent of Ru(G) is at most s.
Proof.
Let B and m be as in Lemma 3.7. Since G is smooth, it is enough to consider elements of G(kˉ), which we can identify with G′(B). By embedding G′ into GLr for some r,
we may assume that the elements of interest are matrices with entries in B,
and we may identify points of the unipotent radical
as the kernel of the map G′(B)→G′(kˉ) given by reduction modulo m.
Then a typical element of the unipotent radical has the form I+M, where I is the r×r identity matrix and M is an r×r matrix with entries in m.
We are therefore after a pth power ps which kills all such matrices M—for then (I+M)ps=I+Mps=I in all cases.
Now note that the entries of a power Mps are homogeneous polynomials in the entries of M of degree ps.
Since mn=0, all such polynomials vanish as soon as ps is at least n.
Hence, if we choose s as in the statement, we are done.
∎
The following example shows that the bound provided by Lemma 4.1 is sharp when the rank of G′ is large enough.
Example 4.2**.**
Suppose G′=GLn where n is as above.
Then we can find elements m1,…,mn−1∈m such that m1⋯mn−1=0,
and the element
[TABLE]
has xn−1=0, so the bound in Lemma 4.1 cannot be improved in this case.
In contrast to the above example, we can see in some easy examples that the bound provided by Lemma 4.1 can be much
too large.
Example 4.3**.**
(i). Suppose G=Rk′/k(GL2) when p=2 and k′/k is a purely inseparable field extension of exponent 1
(recall that the exponent of such a purely inseparable extension is the minimal e such that xpe∈k for all x∈k′).
The fact that k′/k has exponent 1 means in this case that m2=0 for all m∈m, irrespective of the value of n.
Therefore, if we consider any four elements m1,m2,m3,m4∈m arranged in a 2×2 matrix
[TABLE]
we have x4=0, so the maximal order of elements in Ru(G) is 4 in this situation.
However, we can make the minimal n such that mn=0 as large as we like (for example,
by letting k be a field of rational functions in several variables
T1,T2,… and then adjoining elements ti with ti2=Ti for each i).
(ii). Suppose G=Rk′/k(Gm).
If the exponent of the extension k′/k is e, then because the pe power map sends (k′)× to k×,
we see that elements of Ru(G) have order at most pe, and some elements do indeed have this order (by the argument for GLr above, taking r=1).
Hence, in this case, the exponent of Ru(G) coincides with the exponent of the extension k′/k.
Motivated by the examples above, which show dependence on the exponent of the extension k′/k,
we finish with a bound for matrices which depends on that exponent and the rank of the matrices, rather than the number n.
Lemma 4.4**.**
Suppose k′/k has exponent e, and let G=Rk′/k(GLr).
Then the exponent of Ru(G) is at most s,
where s is chosen so that ps≥r2(pe−1).
In particular, if p≥r2, then this exponent is at most e+1.
Proof.
As before, we are after a power ps which kills all r×r matrices M with entries in m.
Since the exponent is e, it is true that mpe=0 for all m∈m.
Again observe that a power Mps has entries which are homogeneous polynomials of degree ps
in the r2 entries of M.
If we take ps large enough so that any monomial of degree ps in r2 variables must contain at least one of the variables at least pe times, then we know that Mps=0.
The claimed bound now follows.
∎
Remarks 4.5*.*
A few comments on this last result:
(i)
When p=2, e=1 and r=2 in Lemma 4.4, we obtain the bound 4=pe+1 which was observed in Example 4.3(i).
On the other hand, for larger e we have to go up to pe+2.
(ii)
When r=1 in Lemma 4.4, we obtain the bound pe which was already observed in Example 4.3(ii).
(iii)
The bound from Lemma 4.1 will obviously be much better in some cases than that provided by Lemma 4.4. The tension between these two observations seems to be something which merits further study, and we will return to it in future work.
(iv)
Computer calculations suggest that if G:=Rk′/k(G′) then the exponent of Ru(Gkˉ) is always the same as the exponent of Ru(Gkˉ)∩Bkˉ, where B:=Ru(Rk′/k(B′)) for B′=T′⋉U′ a Borel subgroup of G′ with split maximal torus T′ (recall we assumed k to be separably closed). We do not know a proof that these exponents are the same—assuming, of course, that it is even true. In any case, one can make a little more conceptual progress in obtaining an upper bound for the exponent of Ru(Gkˉ)∩Bkˉ, as follows.
The group B is connected and solvable (since B′ is), so any unipotent subgroup of Bkˉ is contained in Ru(Bkˉ). In particular, Ru(Gkˉ)∩Bkˉ is contained in Ru(Bkˉ). We now give an upper bound for the exponent of the latter. Observe that B≅C⋉U, where C:=Rk′/k(T′) and U:=Rk′/k(U′). Then Ru(Bkˉ)=Ru(Ckˉ)⋉Ukˉ. Now from Example 4.3(ii) we get that the exponent of Ru(Ckˉ) is precisely e, where e is the exponent of k′/k. Thus the pe-power map sends Ru(Bkˉ) into Ukˉ; denote the image of this map by J. One knows that the exponent of U′ is the smallest integer s such that ps>h−1, where h is the Coxeter number of G′; see [Tes95, Order Formula 0.4]. Thus the ps-power map on U′ factors through 1, and so the ps-power map on U=Rk′/k(U′) also factors through 1. Since J⊆Ukˉ, the exponent of J is at most s. So one gets an upper bound of e+s for the exponent of Ru(Bkˉ) (and hence for the exponent of Ru(Gkˉ)∩Bkˉ), though this bound can be further improved with knowledge of the structure of k′.
Elementary calculations show that when G′=GL2, we have J=1 when k′/k is primitive, giving e as the exponent, and J=1 when k′/k is imprimitive; since all elements of J have order p, we then get e+1 as the exponent. To explain what happens in the imprimitive case, find t∈k′ with exponent e in k′/k; since k′ is imprimitive, we may find also u∈k′∖k(t). One checks
[TABLE]
More generally we ask
Question 4.6**.**
Suppose G′ is not unusual and let r=logp([k′:k(k′)p])−1. Let s=max{⌈logp(hL′−1)⌉} where the maximum is over all Coxeter numbers hL′ of Levi subgroups L′ of G′ with rank at most r. Is the exponent of Ru(Bkˉ) equal to max{e+s,⌈logp(hG′−1)⌉}?
Remark 4.7*.*
Note that the bounds above fail in the context of a general standard pseudo-reductive group. For instance, given a finite purely inseparable field extension k′/k with exponent e, we can take G to be the standard group arising from the 4-tuple (G′,k′/k,T′,C), where G′=T′=1 and C=Rk′′/k(Gm), with k′′/k a finite purely inseparable field extension of arbitrarily large exponent f: for then G≅C has exponent f by Example 4.3(ii).
Acknowledgements:
Part of the research for this paper was carried out while the
authors were staying at the Mathematical Research Institute
Oberwolfach supported by the “Research in Pairs” programme.
The authors also acknowledge the financial support of EPSRC Grant EP/L005328/1 and Marsden Grant UOA1021.
We thank Brian Conrad for comments and discussion. We thank Gopal Prasad for some helpful hints to improve the results. We are also grateful to the referee for their comments.
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