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A L

E S

E D L ’IN IT ST T U

F O U R

ANNALES

DE

L’INSTITUT FOURIER

Karin BAUR & Anne MOREAU

Quasi-reductive (bi)parabolic subalgebras in reductive Lie algebras.

Tome 61, no2 (2011), p. 417-451.

<http://aif.cedram.org/item?id=AIF_2011__61_2_417_0>

© Association des Annales de l’institut Fourier, 2011, tous droits réservés.

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QUASI-REDUCTIVE (BI)PARABOLIC SUBALGEBRAS IN REDUCTIVE LIE ALGEBRAS.

by Karin BAUR & Anne MOREAU (*)

Abstract. — We say that a finite dimensional Lie algebra is quasi-reductive if it has a linear form whose stabilizer for the coadjoint representation, modulo the center, is a reductive Lie algebra with a center consisting of semisimple elements.

Parabolic subalgebras of a semisimple Lie algebra are not always quasi-reductive (except in types A or C by work of Panyushev). The classification of quasi-reductive parabolic subalgebras in the classical case has been recently achieved in unpub- lished work of Duflo, Khalgui and Torasso. In this paper, we investigate the quasi- reductivity of biparabolic subalgebras of reductive Lie algebras. Biparabolic (or seaweed) subalgebras are the intersection of two parabolic subalgebras whose sum is the total Lie algebra. As a main result, we complete the classification of quasi- reductive parabolic subalgebras of reductive Lie algebras by considering the excep- tional cases.

Résumé. — Une algèbre de Lie de dimension finie est dite quasi-réductive si elle possède une forme linéaire dont le stablisateur pour la représentation coadjointe, modulo le centre, est une algèbre de Lie réductive avec un centre formé d’éléments semi-simples. Les sous-algèbres paraboliques d’une algèbre de Lie semi-simple ne sont pas toujours quasi-réductives (sauf en types A ou C d’après un résultat de Pa- nyushev). Récemment, Duflo, Khalgui and Torasso ont terminé la classification des sous-algèbres paraboliques quasi-réductives dans le cas classique. Dans cet article nous étudions la quasi-réductivité des sous-algèbres biparaboliques des algèbres de Lie réductives. Les sous-algèbres biparaboliques sont les intersections de deux sous-algèbres paraboliques dont la somme est l’algèbre de Lie ambiante. Notre prin- cipal résultat est la complétion de la classification des sous-algèbres paraboliques quasi-réductives des algèbres de Lie réductives.

Keywords:Reductive Lie algebras, quasi-reductive Lie algebras, index, biparabolic Lie algebras, seaweed algebras, regular linear forms.

Math. classification:17B20, 17B45, 22E60.

(*) We thank M. Duflo for introducing us to the subject of quasi-reductive subalgebras.

We also thank P. Tauvel and R.W.T. Yu for useful discussions. Furthermore, we thank W. de Graaf and J. Draisma for helpful hints in the use ofGAP. At this point, we also want to thank the referee for the very useful comments and suggestions. This work was supported by the Swiss National Science Foundation (grant PP0022-114794).

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Introduction

LetGbe a complex connected linear algebraic Lie group. Denote bygits Lie algebra. The groupGacts on the dualg ofgby the coadjoint action.

Forf ∈g, we denote by G(f) its stabilizer inG; it always contains the centerZofG. One says that a linear formf ∈ghasreductive type if the quotient G(f)/Z is a reductive subgroup of GL(g). The Lie algebra g is calledquasi-reductive if it has linear forms of reductive type. This notion goes back to M. Duflo. He initiated the study of such Lie algebras because of applications in harmonic analysis, see [3]. For more details about linear forms of reductive type and quasi-reductive Lie algebras we refer the reader to Section 1.

Reductive Lie algebras are obviously quasi-reductive Lie algebras since in that case, 0 is a linear form of reductive type. Biparabolic subalgebras form a very interesting class of non-reductive Lie algebras. They naturally extend the classes of parabolic subalgebras and of Levi subalgebras. The latter are clearly quasi-reductive since they are reductive subalgebras.. Biparabolic subalgebras were introduced by V. Dergachev and A. Kirillov in the case g = sln, see [2]. A biparabolic subalgebra or seaweed subalgebra (of a semisimple Lie algebra) is the intersection of two parabolic subalgebras whose sum is the total Lie algebra.

In this article, we are interested in the classification of quasi-reductive (bi)parabolic subalgebras. Note that it is enough to consider the case of (bi)parabolic subalgebras of the simple Lie algebras, cf. Remark 1.4.

In the classical cases, various results are already known: All biparabolic subalgebras ofslnandsp2nare quasi-reductive as has been proven by D. Pa- nyushev in [19]. The case of orthogonal Lie algebras is more complicated:

On one hand, there are parabolic subalgebras of orthogonal Lie algebras which are not quasi-reductive, as P. Tauvel and R.W.T. Yu have shown (Section 3.2 of [20]). On the other hand, D. Panyushev and A. Dvorsky exhibit many quasi-reductive parabolic subalgebras in [6] and [19] by con- structing linear forms with the desired properties. Recently, M. Duflo, M.S. Khalgui and P. Torasso have obtained the classification of quasi- reductive parabolic subalgebras of the orthogonal Lie algebras in unpub- lished work, [4]. They were able to characterize quasi-reductive parabolic subalgebras in terms of the flags stabilized by the subalgebras.

The main result of this paper is the completion of the classification of quasi-reductive parabolic subalgebras of simple Lie algebras. This is done in Section 5 (Theorem 5.1 and Theorem 5.2). Our goal is ultimately to de- scribe all quasi-reductive biparabolic subalgebras. Thus, in the first sections

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we present results concerning biparabolic subalgebras to remain in a gen- eral setting as far as possible. For the remainder of the introduction,gis a finite dimensional complex semisimple Lie algebra.

The paper is organized as follows:

In Section 1 we introduce the main notations and definitions. We also include in this section a short review of known results about biparabolic subalgebras, including the description of quasi-reductive parabolic subalge- bras in the classical Lie algebras (Subsection 1.4). In Section 2, we describe two methods of reduction, namely the transitivity property (Theorem 2.1) and the additivity property (Theorem 2.11). As a first step of our classifica- tion, we exhibit in Section 3 a large collection of quasi-reductive biparabolic subalgebras ofg (Theorem 3.6). Next, in Section 4, we consider the non quasi-reductive parabolic subalgebras ofg, for simplegof exceptional type (Theorems 4.1, 4.3 and 4.6). This is a crucial part of the paper. Indeed, to study the quasi-reductivity, we can make explicit computations (cf. Sec- tion 5) while it is much trickier to prove that a Lie algebra is not quasi- reductive. Using the results of Sections 2, 3 and 4, we are able to cover a large number of parabolic subalgebras. The remaining cases are dealt with in Section 5 (Theorem 5.6, Propositions 5.8 and 5.9). This completes the classification of quasi-reductive parabolic subalgebras of g(Theorems 5.1 and 5.2, see also Tables 5.1 and 5.2).

At this place, we also want to point out that in [16], O. Yakimova and the second author study themaximal reductive stabilizersof quasi-reductive parabolic subalgebras of g. This piece of work yields an alternative proof of Proposition 5.9 which is not based on the computer programmeGAP, see Remark 5.10.

1. Notations, definitions and basic facts

In this section, we recall a number of known results that will be used in the sequel.

1.1.Letgbe a complex Lie algebra of a connected linear algebraic Lie groupG. Denoting by g(f) the Lie algebra ofG(f), we have g(f) ={x∈ g| (adx)(f) = 0} where ad is the coadjoint representation of g. Recall that a linear formf ∈g is of reductive typeifG(f)/Z is a reductive Lie subgroup of GL(g). We can reformulate this definition as follows:

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Definition 1.1. — An elementf of g is said to be of reductive type if g(f)/z is a reductive Lie algebra whose center consists of semisimple elements ofgwherezis the center ofg.

Recall that a linear form f ∈ g is regular if the dimension of g(f) is as small as possible. By definition, theindex ofg, denoted by indg, is the dimension of the stabilizer of a regular linear form. The index of various special classes of subalgebras of reductive Lie algebras has been studied by several authors, cf. [18], [25], [14], [15]. For the index of seaweed algebras, we refer to [17], [6], [20], [22], [10] and [11].

Recall that gis calledquasi-reductive if it has linear forms of reductive type. From Duflo’s work [3, §§I.26-27] one deduces the following result about regular linear forms of reductive type:

Proposition 1.2. — Suppose thatgis quasi-reductive. The set of reg- ular linear forms of reductive type forms a Zariski open dense subset ofg. 1.2.From now on, gis a complex finite dimensional semisimple Lie al- gebra. The dual ofgis identified withgthrough the Killing form ofg. For u∈ g, we denote by ϕu the corresponding element of g. For u ∈g, the restriction ofϕu, to any subalgebraa ofgwill be denoted by (ϕu)|a.

Denote by π the set of simple roots with respect to a fixed triangular decomposition

g=n+⊕h⊕n

of g, and by ∆π (respectively ∆+π, ∆π) the corresponding root system (respectively positive root system, negative root system). Ifπ0 is a subset ofπ, we denote by ∆π0 the root subsystem of ∆π generated byπ0 and we set ∆±π0 = ∆π0 ∩∆±π. For α∈ ∆π, denote by gα the α-root subspace of gand lethα be the unique element of [gα,g−α] such that α(hα) = 2. For eachα∈∆π, fixxα∈gαso that the family {xα, hβ ; α∈∆π, βπ}is a Chevalley basis ofg. In particular, for non-colinear rootsαandβ, we have [xα, xβ] =±(p+ 1)xα+β ifβis the source of the α-string throughβ. We briefly recall a classical construction due to B. Kostant. It associates to a subset of π a system of strongly orthogonal positive roots in ∆π. This construction is known to be very helpful to obtain regular forms on biparabolic subalgebras ofg. For a recent account about thecascade con- struction of Kostant, we refer to [22, §1.5] or [21, §40.5].

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Forλinhandα∈∆π, we shall writehλ, αiforλ(hα). Recall that two rootsαandβ in ∆πare said to be strongly orthogonalif neitherα+β nor αβ is in ∆π. Let π0 be a subset of π. The cascadeKπ0 of π0 is defined by induction on the cardinality ofπ0 as follows:

(1) K(∅) =∅,

(2) Ifπ01,. . . ,πr0 are the connected components ofπ0, thenKπ0 =Kπ10

· · · ∪Kπ0r,

(3) If π0 is connected, then Kπ0 = {π0} ∪KT where T = {α ∈ π0 | hα, επ0i= 0}andεπ0 is the highest positive root of ∆+π0.

ForK∈Kπ0, set

ΓK ={α∈∆K | hα, εKi>0} and Γ0K= ΓK\ {εK}. Notice that the subspace P

K∈ΓK

gαis a Heisenberg Lie algebra whose center isgεK.

The cardinality kπ of Kπ only depends on g; it is independent of the choices of hand π. The values of kπ for the different types of simple Lie algebras are given in Table 1.1; in this table, for a real numberx, we denote by [x] the largest integer6x.

A`, `>1 B`, `>2 C`, `>3 D`, `>4 G2 F4 E6 E7 E8

`+ 1 2

` ` 2

` 2

2 4 4 7 8

Table 1.1. kπ for the simple Lie algebras.

For π0 a subset of π, we denote by Eπ0 the set of the highest rootsεK whereKruns over the elements of the cascade ofπ0. By construction, the subsetEπ0 is a family of pairwise strongly orthogonal roots in ∆π0. For the convenience of the reader, the setEπ, for each simple Lie algebra of type π, is described in the Tables 1.2 and 1.3. We denote byEπ0 the subspace ofh which is generated by the elements ofEπ0.

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A`, `>1:

α1 α2 α−1 αi = αi + · · · + αi+(`−2i+1), i6

`+ 1 2

}

B`, `>2 :

α1 α2 α−1 α

>

i = αi−1+ 2αi+· · ·+ 2α`, ieven, i6`} ∪ {εi= αi, iodd, i6`}

C`,`>3:

α1 α2 α−1 α

<i= 2αi+· · ·+ 2α`−1+ α`, i6`−1} ∪ {ε`=α`}

D`,`even,`>4:

α1 α2 α−2

α

α−1

i = αi−1 + 2αi +

· · · + 2α`−2 + α`−1 + α`, ieven, i < `−1} ∪ {εi=αi, iodd, i < `} ∪ {ε`=α`}

D`,`odd,`>5:

α1 α2 α−2

α

α−1

i = αi−1 + 2αi +

· · · + 2α`−2 + α`−1 + α`, ieven, i < `−1} ∪ {εi=αi, iodd, i < `} ∪`−1=α`−2`−1+α`} Table 1.2. Eπ for the classical Lie algebras.

1.3.Abiparabolicsubalgebra ofgis defined to be the intersection of two parabolic subalgebras whose sum isg. This class of algebras has first been studied in the case ofsln by Dergachev and Kirillov [2] under the name of seaweedalgebras.

For a subsetπ0ofπ, we denote byp+π0 the standard parabolic subalgebra of gwhich is the subalgebra generated by b+ = h⊕n+ and by g−α, for απ0. We denote by pπ0 the “opposite parabolic subalgebra” generated by b = n⊕h and by gα, for απ0. Set lπ0 = p+π0 ∩pπ0. Then lπ0 is a Levi factor of both parabolic subalgebrasp+π0 and pπ0 and we can write lπ0 = n+π0 ⊕h⊕nπ0 where n±π0 = n±∩lπ0. Let m+π0 (respectively mπ0) be the nilradical of p+π0 (respectively pπ0). We denote by gπ0 the derived Lie algebra oflπ0 and byz(lπ0) the center oflπ0. The Cartan subalgebrah∩gπ0 ofgπ0 will be denoted byhπ0.

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G2:

α1 α2

>1= 23, ε2= 01}

F4: α1 α2 > α3 α41= 2342, ε2= 0122, ε3= 0120, ε4= 0100}

E6: α1 α3 α4 α5 α6

α2

1= 12321 2

, ε2= 11111 0

, ε3= 01110

0

, ε4= 00100 0

}

E7: α1 α3 α4 α5 α6 α7

α2

α1

1= 234321 2

, ε2= 012221 1

, ε3= 012100

1

, ε4= 000001 0

, ε5= 000000

1

, ε6= 010000 0

, ε7= 000100

0 }

E8: α1 α3 α4 α5 α6 α7 α8

α2

1= 2465432 3

, ε2= 2343210 2

, ε3= 0122210

1

, ε4= 0121000 1

, ε5= 0000010

0

, ε6= 0000000 1

, ε7= 0100000

0

, ε8= 0001000 0

}

Table 1.3. Eπ for the exceptional Lie algebras.

Definition 1.3. — The subalgebraqπ12 of ggiven as follows by the subsetsπ1, π2π

qπ12:=p+π1∩pπ2=n+π2⊕h⊕nπ1

is called thestandardbiparabolic subalgebra (associated toπ1andπ2). Its nilpotent radical isuπ12 := (n+π

2∩m+π

1)⊕(nπ

1∩mπ

2)andlπ12 :=lπ1∩π2 is the standard Levi factor ofqπ12.

Any biparabolic subalgebra is conjugate to a standard one, see [22, §2.3]

or [10, §2.5]. So, for our purpose, it will be enough to consider standard biparabolic subalgebras.

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Remark 1.4. — The classification of quasi-reductive (bi)parabolic sub- algebras of reductive Lie algebras can be deduced from the classification of quasi-reductive (bi)parabolic subalgebras of simple Lie algebras: A sta- bilizer of a linear form on g is the product of its components on each of the simple factors of gand of the center of g. As a consequence, we may assume thatgis simple without loss of generality.

Letπ1, π2be two subsets ofπ. The dual ofqπ12is identified toqπ21via the Killing form ofg. Fora= (aK)K∈Kπ

2 ∈(C)kπ2 andb= (bL)L∈Kπ

1 ∈ (C)kπ1, set

u(a, b) = X

K∈Kπ2

aKx−εK+ X

L∈Kπ1

bLxεL

It is an element ofuπ21 and the linear form (ϕu)|qπ12 is a regular ele- ment ofqπ12 for any (a, b) running through a nonempty open subset of (C)kπ2+kπ1, cf. [22, Lemma 3.9].

We denote by Eπ12 the subspace generated by the elements εK, for K∈Kπ1∪Kπ2. Thus, dimEπ12 = kπ1+ kπ2−dim(Eπ1Eπ2). As it has been proved in [10, §7.16], we have

indqπ12 = (rkg−dimEπ12) + (kπ1+ kπ2−dimEπ12) (1.1)

Remark 1.5. — By (1.1), the index of qπ12 is zero if and only if Eπ1Eπ2 = {0} and kπ1 + kπ2 = rkg. For example, in type E6, there are exactly fourteen standard parabolic subalgebrasp+π0 with index zero.

The corresponding subsetsπ0πof the simple roots are the following:

1, α5};{α3, α6};{α1, α4, α5};{α3, α4, α6};{α1, α5, α6};

1, α3, α6};{α1, α3, α5};{α3, α5, α6};{α1, α3, α4};{α4, α5, α6};

1, α3, α4, α5};{α3, α4, α5, α6};{α1, α2, α3, α4};{α2, α4, α5, α6}.

This was already observed in the unpublished work [7] of A. Elashvili (with a small error).

In the sequel, we will often make use of the following element of uπ21 on our way to construct reductive forms:

uπ12 = X

ε∈Eπ2,ε /∈∆+π1

x−ε

Ifπ2=π, we simply writeuπ

1 foruπ

1 and, in the special case ofπ1=∅ andπ2=π, we writeu foru. LetB be the Borel subgroup ofGwhose Lie algebra isb+. We summarize in the following proposition useful results of Kostant concerning the linear form (ϕu)|b+. They can be found in [21, Proposition 40.6.3].

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Proposition 1.6. — (i)The linear form(ϕu)|b+ is of reductive type for b+. More precisely, the stabilizer of ϕu in b+ is the subspace

T

K∈Kπ

kerεK ofhof dimensionrkg−kπ.

(ii) Letm be an ideal ofb+ contained inn+. TheB-orbit ofu)|m in m is an open dense subset ofm.

1.4.We end the section by reviewing what is known in the classical case.

First recall that the biparabolic subalgebras of simple Lie algebras of type A and C are always quasi-reductive as has been shown by D. Panyushev in [19].

The classification of quasi-reductive parabolic subalgebras of the orthog- onal Lie algebras is given in the recent work [4] of Duflo, Khalgui and Torrasso. Since we will use this result repeatedly, we state it below.

Let E be a complex vector space of dimension N endowed with a non- degenerate symmetric bilinear form. Denote bysoN the Lie algebra of the corresponding orthogonal group. LetV={{0}=V0(V1(· · ·(Vs=V} be a flag of isotropic subspaces in E, with s > 1. Its stabilizer in soN

is a parabolic subalgebra of soN and any parabolic subalgebra of soN is obtained in this way. We denote bypV the stabilizer ofVinsoN.

Theorem 1.7. — [4] Let V = {{0} = V0 ( V1 ( · · · ( Vs = V} be a flag of isotropic subspaces in E with s > 1. Denote by V0 the flag of isotropic subspaces in E which is equal to V\ {V} if dimV is odd and equal toN/2, and equal toVotherwise.

The Lie algebrapV is quasi-reductive if and only if the sequenceV0 does not contain two consecutive subspaces of odd dimension.

Example 1.8. — Forg=D6 there are twelve standard parabolic subal- gebrasp =p+π0 which are not quasi-reductive. The corresponding subsets π0πof the simple roots are the following:

2},{α4},{α1, α4},{α2, α4},{α2, α5},{α2, α6}, {α1, α2, α4},{α2, α3, α4},{α2, α4, α5},{α2, α4, α6}, {α2, α5, α6},{α2, α4, α5, α6}.

Among these, the connectedπ0 are{α2},{α4},{α2, α3, α4}.

Thus it remains to determine the quasi-reductive parabolic subalgebras of the exceptional Lie algebras. This is our goal.

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2. Methods of reduction

In this section, we develop methods of reduction to deduce the quasi- reductivity of a parabolic subalgebra from the quasi-reductivity of other subalgebras. We assume thatπ2 =π. Nevertheless we keep the notations of biparabolic subalgebras where it is convenient.

2.1.The following theorem seems to be standard. As there is no proof to our knowledge, we give a short proof here:

Theorem 2.1(Transitivity). — Letπ00, π0be subsets ofπwithπ00π0. Suppose thatKπ0 ⊂Kπ. Then,qπ00is quasi-reductive if and only ifqπ000

is.

Proof. — Note that the assumption Kπ0 ⊂ Kπ implies indqπ000 = indqπ00+ (kπ−kπ0) by formula (1.1). Sinceuπ0 is an ideal ofb+ con- tained in n+, Proposition 1.6(ii) enables to choose w0 in lπ0 such that both (ϕw0+u

π0)|qπ00 and (ϕw0)|qπ000 are regular linear forms ofqπ00 and qπ000 respectively. Then one can show thatqπ000w0) =qπ00w0+u

π0)⊕

P

K∈Kπ\Kπ0

ChεK. By Proposition 1.2, ifqπ00 (respectivelyqπ000) is quasi- reductive, then we can assume furthermore that (ϕw0+u

π0)|qπ00 (respec- tively (ϕw0)|qπ000) has reductive type. Hence the equivalence of the theo-

rem follows.

Suppose that gis simple and let eπbe the subset of π defined byKπ = {π} ∪K

eπ

. Ifgis of exceptional type,π\πeonly consists of one simple root which we denote byαπ. Note thatαπ is the simple root which is connected to the lowest root in the extended Dynkin diagram.

As a consequence of Theorem 2.1, to describe all the quasi-reductive par- abolic subalgebras ofg, forgof exceptional type, it suffices to consider the case of parabolic subalgebrasp+π0 withαππ0. This will be an important reduction in the sequel.

Remark 2.2. — If g has type F4 (resp. E6, E7, E8), then g eπ

has type C3 (resp. A5, D6, E7). In particular, if g has type F4 or E6, then p+π0 is quasi-reductive for any π0 which does not containαπ because in types A and C all (bi)parabolic subalgebras are quasi-reductive.

2.2.As a next step we now focus on a property that we call “additivity”

to relate the quasi-reductivity of different parabolic subalgebras (cf. Theo- rem 2.11). Throughout this paragraph,gis assumed to be simple.

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Definition 2.3. — Let π0, π00 be subsets of π. We say that π0 is not connected toπ00ifα0 is orthogonal toα00, for all(α0, α00)in π0×π00.

Notation 2.4. — For a positive root α, we denote byKπ+(α) the only elementLofKπ such thatα∈ΓL. Note that unlessα∈Eπ,Kπ+(α) is the only elementLofKπ for whichεLαis a positive root. ForK∈Kπ, we haveKπ+K) =K.

Remark 2.5. — It can be checked thatKπ+(α) =Kπ+(β) forα,β simple if and only ifαandβare in the same orbit of−w0wherew0is the longest element of the Weyl group ofg. This suggests thatw0 should play a role in these questions, as may be guessed from a result of Kostant which says that Eπ is a basis of the space of fixed points of −w0 and from work of Joseph and collaborators ([10, 11]).

Definition 2.6. — We shall say that two subsets π0, π00which are not connected to each othersatisfy the condition (∗)if:

(∗) Kπ+0)6=Kπ+00) ∀(α0, α00)∈π0×π00.

Note that if kπ = rkg(that is if−w0acts trivially onπ), the condition (∗) is always satisfied. Moreover, by using Table 1.3, a case-by-case discussion shows:

Lemma 2.7. — Assume thatgis simple of exceptional type and letπ0 be a connected subset of π containing απ. Then, for any subset π00 of π which is not connected toπ0, the two subsets π0, π00 satisfy the condition (∗), unless g= E6,π0 ={α1, α2, α3, α4} and π00 ={α6} or by symmetry π0={α2, α4, α5, α6} andπ00={α1}.

Remark 2.8. — If g= E6, with π0 ={α1, α2, α3, α4} and π00 ={α6}, then Kπ+1) = Kπ+6) = {{α1, α3, α4, α5, α6}}, so π0 and π00 do not satisfy the condition (∗). As a matter of fact, the parabolic subalgebra p+π0∪π00 will appear as a very special case (see Remark 2.12).

Letπ0, π00be two subsets ofπwhich are not connected to each other and assume thatπ0, π00satisfy condition (∗). By Proposition 1.6(ii), we can let w0be in lπ0 such that (ϕw)|p+

π0 is regular wherew=w0+uπ0. Denote bys0 be the image ofp+π0w) by the projection map fromp+π0 to its derived Lie algebragπ0⊕m+π0 with respect to the decompositionp+π0=z(lπ0)⊕gπ0⊕m+π0. Letk0 be the intersection of z(lπ0) with T

ε∈Eπ, ε6∈∆+

π0

kerε.

Lemma 2.9. — (i) indp+π0 = dims0+ dimk0. (ii) [s0,p+π0∪π00]⊂p+π0 andϕw([s0,p+π0∪π00]) ={0}.

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Proof. — (i) We have dimp+π0w) = indp+π0. Since the image ofp+π0w) by the projection map from p+π0 to gπ0 ⊕m+π0 is s0, it suffices to observe that the intersection ofz(lπ0) withp+π0w) isk0. And this follows from the choice ofw.

(ii) Letxbe an element ofp+π0w); writex=x0+x0+x+withx0∈z(lπ0), x0∈gπ0 andx+∈m+π0. Since [x+, w0] lies inm+π0, the fact thatx∈p+π0w) means [x0, uπ0] + [x0, w0] + [x0, uπ0] + [x+, uπ0]∈m+π0. First, we have to show [x0+x+,p+π0∪π00]⊂p+π0. As [x0,p+π0∪π00]⊂p+π0 sinceπ00, π0 are not connected, it suffices to prove thatx+ ∈m+π0∪π00. If not, there areγ∈∆+π00,K ∈Kπ, andα0 ∈∆+π0 such that

γεK+

π(γ)=−(α0+εK) , i.e.εK+

π(γ)=γ+ (α0+εK) Henceγ, α0 ∈Γ0K+

π(γ)that isKπ+0) =Kπ+(γ). But this contradicts condi- tion (∗). Thus [x0+x+,p+π0∪π00]⊂p+π0.

It remains to show: ϕw([x0+x+,p+π0∪π00]) = {0} that is [x0+x+, w] ∈ m+π0∪π00. If [x0+x+, w] 6∈m+π0∪π00, there must be γ ∈ ∆+π \∆π0, K ∈Kπ, andα00 ∈∆+π00 such that γεK =α00. In particular α00 ∈ Γ0

Kπ+(γ) that is Kπ+00) =Kπ+(γ). On the other hand, [x, w]∈m+π0 implies that there exist α0 ∈∆+π0 andL∈Kπ, such that

γεK+

π(γ)=−(α0+εL) , i.e.εK+

π(γ)=γ+ (α0+εL) As before, we deduce that α0 ∈Γ0K+

π(γ), i.e.Kπ+0) =Kπ+(γ) =Kπ+00)

and this contradicts condition (∗).

Corollary 2.10. — Letπ0, π00 be two subsets ofπwhich are not con- nected to each other and satisfy condition(∗). Ifp+π0∪π00 is quasi-reductive thenp+π0 andp+π00 are both quasi-reductive.

Proof. — Suppose thatp+π0∪π00is quasi-reductive and that any one of the other two parabolic subalgebras is not quasi-reductive and show that this leads to a contradiction. By assumption we can choose ϕ ∈ (p+π0∪π00) of reductive type for p+π0∪π00 such that ϕ0 = ϕ|

p+ π0

and ϕ00 = ϕ|

p+ π00

are p+π0- regular andp+π00-regular respectively. Suppose for instance that p+π0 is not quasi-reductive. By Proposition 1.6(ii) we can suppose furthermore that ϕ0 = (ϕw)|p+

π0 for somew=w0+uπ0 withw0∈lπ0.

Since we assumed that p+π0 is not quasi-reductive, (ϕw)|p+

π0 contains a nonzero nilpotent element, x, which is so contained in the derived Lie algebra of p+π0. Then, Lemma 2.9(ii) gives [x,p+π0∪π00] ⊂ p+π0 and {0} = ϕw([x,p+π0∪π00]) = ϕ0([x,p+π0∪π00]) = ϕ([x,p+π0∪π00]). As a consequence, p+π0∪π00(ϕ) contains the nonzero nilpotent elementx. This contradicts the

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choice ofϕ. The same line of arguments works if we assume thatp+π00 is not

quasi-reductive.

Under certain conditions, the converse of Corollary 2.10 is also true as we show now. To begin with, let us express the index ofp+π0∪π00in terms of those ofp+π0 andp+π00. AsEπ0∪π00=Eπ0+Eπ0, we get: dimEπ0∪π00= dimEπ0+ dimEπ00−dim(Eπ0Eπ00). Hence, formula (1.1) implies indp+π0∪π00 = indp+π0+ indp+π00−(rkg+ kπ−2 dim(Eπ0Eπ00)) . (2.1)

In case rkg= kπ, the intersection Eπ0Eπ00 is equal to Eπ and has dimension rkg. Hence, the index is additive in that case, as (2.1) shows.

Theorem 2.11 (Additivity). — Assume thatgis simple and of excep- tional type and that kπ = rkg. Let π0, π00 be two subsets of π which are not connected to each other. Then,p+π0∪π00 is quasi-reductive if and only if bothp+π0 andp+π00 are quasi-reductive.

Remark 2.12. — The conclusions of Theorem 2.11 is valid for classical simple Lie algebras, even without the hypothesis kπ = rkg. In types A or C this follows from the fact that all biparabolic subalgebras are quasi- reductive. Ifgis an orthogonal Lie algebra, this is a consequence of Theo- rem 1.7. However, for the exceptional Lie simple algebra E6, the only one for which kπ6= rkg, the conclusions of Theorem 2.11 may fail. Indeed, let us consider the following subsets ofπforgof type E6:π0={α1, α2, α3, α4} andπ00={α6}.. By Remark 1.5,p+π0 is quasi-reductive as a Lie algebra of zero index. On the other hand, p+π00 is quasi-reductive by the transitivity property, cf. Remark 2.2. But, it will be shown in Theorem 4.6 thatp+π0∪π00

is not quasi-reductive.

As a consequence of Lemma 2.7 and Corollary 2.10, even in type E6

where rkg 6= kπ, if p+π0∪π00 is quasi-reductive, then p+π0 and p+π00 are both quasi-reductive.

As a by-product of our classification, we will see that the above situation is the only case which prevents the additivity property to be true for all simple Lie algebras (see Remark 5.3).

Proof. — We argue by induction on the rank of g. By the transitivity property (Theorem 2.1), Remark 2.12 and the induction, we can assume that αππ0. Then, by Lemma 2.7 and Corollary 2.10, only remains to prove that if bothp+π0 andp+π00 are quasi-reductive, then so isp+π0∪π00.

Assume that both p+π0 and p+π00 are quasi-reductive. By Proposition 1.2, we can find a linear regular formϕin (p+π0∪π00) such that ϕ0 =ϕ|

p+ π0

and

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ϕ00=ϕ|

p+ π00

are regular and of reductive type forp+π0 andp+π00 respectively.

By Proposition 1.6(ii), we can assume thatϕ= (ϕw+u)|p+

π0 ∪π00, wherew= h+w0+w00, withw0 ∈n+π0,w00∈n+π00andh∈h. Hence,ϕ0= (ϕh+w0+u)|p+

π0

andϕ00= (ϕh+w00+u)|p+ π00.

Use the notations of Lemma 2.9. By Lemma 2.9(ii), s0 is contained in p+π0∪π00(ϕ). Show now thatk0is zero. Lethbe an elementk0. Sinceh∈k0, we haveε(h) = 0 for anyε∈Eπwhich is not in ∆+π0. On the other hand, for any ε∈Eπ∩∆+π0, we have ε(h) = 0 sincehlies in the center oflπ0. Hence, our assumption rkg= kπimpliesh= 0. As a consequence of Lemma 2.9(i), we deduce that indp+π0 = dims0. Similarly, ifs00 denotes the image ofp+π0000) under the projection fromp+π00 togπ00⊕m+π00, Lemma 2.9(ii) tells us thats00 is contained inp+π0∪π00(ϕ) and that indp+π00= dims00.

To summarize, our discussion shows thats0+s00is contained inp+π0∪π00(ϕ) and that these two subspaces have the same dimension by equation (2.1). So s0+s00=p+π0∪π00(ϕ). But by assumption,s0+s00only consists of semisimple elements. From that we deduce that ϕ is of reductive type for p+π0∪π00,

whence the theorem.

3. Some classes of quasi-reductive biparabolic subalgebras In this section we show that, under certain conditions on the interlace- ment of the two cascades ofπ1andπ2, we can deduce thatqπ12 is quasi- reductive (Theorem 3.6). We assume in this section thatgis simple.

3.1.We start by introducing the necessary notations. Recall that for a positive root α, Kπ+(α) stands for the only element L of Kπ such that α∈ΓL, cf. Notation 2.4. To any positive root α∈∆+π we now associate the subsetKπ(α) of the cascadeKπ of allLsuch that the highest rootεL

can be added toα:

Kπ(α) = {L∈Kπ|εL+α∈∆+π}.

Observe that the setKπ(α) may be empty or contain more than one ele- ment.

Examples 3.1. — (1) IfK is in the cascadeKπ thenKπK) is empty.

(2) In type E7, forα=α4+α5+α6, the set Kπ(α) has more than one element:ε4+α, ε5+α, ε6+αare all positive roots.

We need also the following notation:

∆e+π ={α∈∆+π, α= 1

2(εKεK0) ; K, K0∈Kπ}.

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