C OMPOSITIO M ATHEMATICA
H ISAYOSI M ATUMOTO
C
−∞-Whittaker vectors corresponding to a
principal nilpotent orbit of a real reductive linear Lie group, and wave front sets
Compositio Mathematica, tome 82, n
o2 (1992), p. 189-244
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C- ~-Whittaker
vectorscorresponding
to aprincipal nilpotent
orbit of
areal reductive linear Lie group, and
wavefront
setsHISAYOSI MATUMOTO*
Mathematical Sciences Research Institute, 1000 Centennial Drive, Berkeley CA 94720, U.S.A.
Received 5 March 1990; accepted 23 September 1991 (Ç)
0. Introduction
For an infinite-dimensional admissible irreducible
representation V
ofGL(2, R) (or
moregeneral groups),
a realization of V in the space of(classical)
Whittakerfunctions is called a Whittaker model
([19], etc.).
Whittaker models and their variousgeneralizations
have been studiedby
various mathematicians. Consider-ing
a non-trivial Whittaker vector in the "dual" of V amounts toconsidering
anembedding
of V into "the space of Whittaker functions".To be
precise,
we introduce thefollowing
notations and notions. Let G be areal reductive linear Lie group and let go be its Lie
algebra. (The precise
definition of "a real reductive linear Lie
group"
isgiven
in 1.2. This definition is found in[67].)
We denoteby
g thecomplexification
of go. We fix a maximalcompact subgroup
K of G. Let SP be a minimalparabolic subgroup
and letN
bethe nilradical of the
opposite parabolic subgroup
to ’P. We denoteby
tt thecomplexified
Liealgebra
ofN.
We fix an admissible( = non-degenerate) unitary character 03C8
onN
and denote thecorresponding complexified
differential character of fiby
the same letter. Let M be ag-module
and we call v E M aWhittaker vector if Xv =
03C8(X)v
for all X E fi([36]).
Forquasi-split
groups, in[36],
Kostant studied Whittaker vectors. Inparticular,
Kostantproved
thedimension of the space of Whittaker vectors in the
(algebraic)
dual of the Harish- Chandra module of anon-unitary principal
seriesrepresentation
isequal
to thecardinality
of the littleWeyl
group(say wG). (In
his thesis at MIT([40]), Lynch
extended this result to the
non-quasi-split case.)
In order that a Whittaker vectorv in V*
actually
define a(continuous) homomorphism
of V to the space of Whittakerfunction,
we need to extend v to some continuous linear functional on aG-globalization
of E Let V be a Harish-Chandra(g, K)-module
and we fix anadmissible Hilbert
G-representation H
whose K-finitepart
is V. LetVoo (resp. Vw)
be the space of COO
(resp.
realanalytic)
vectors in H. Casselman and Wallach(respectively, Schmid)
established a remarkableresult; Voo (resp. Vw)
does not* Address from September 1991: Department of Mathematics, SUNY at Stony Brook, Stony Brook, NY 11794-3651.
depend
on the choice of H. We call a Whittaker vector in the continuous dual ofV~ (resp. V03C9)
aC - ’ -(resp. C-03C9)-Whittaker
vector. We denoteby Wh~n,03C8(V) (resp.
Wh03C9n,03C8(V))
the space of c-~(resp.
C-03C9-Whittakervectors).
Goodman andWallach
([12])
observed that every Whittaker vector in V*really
extends to aC-03C9-Whittaker vector for
quasi-split
groups.(Actually, they proved
more. Theirresult is described in terms
of Gevrey vectors.)
For C - °°-Whittaker vectors, the situation isquite
different. As Kostant observed in[36],
a Whittaker vector inthe
algebraic
dual of the Harish-Chandra module of aprincipal
series represen- tation is not necessary to extend to a C" 00 - Whittaker vector.Actually,
theWhittaker vector which has such an extension should come from
(the analytic
continuation
of)
aJacquet integral
studiedby [18], [57], [12],
etc. Aspointed
out in
[12]
and[72],
a C - ~-Whittaker vectorcorresponds
to ahomomorphism
to the space of Whittaker functions
satisfying
certaingrowth
condition.A Harish-Chandra module V is called
quasi-large
if the Gelfand-Kirillov dimensionDim(V)
of V isequal
to dimN.
For the definitionof Dim( ),
see[66].
(If
G isquasi-split, V
isquasi-large
if andonly
if V islarge
in the sense of[66]).
In[46,47],
wegeneralized
some results in[36]
and[12]
tonon-quasi-split
caseand obtained the
following
results.THEOREM A’.
Let .p be
an admissible(= non-degenerate) (unitary)
character onfi and let V be a Harish-Chandra
(g, K)-module. Then,
we haveWh03C9n,03C8(V) ~
0if
and
only if
V isquasi-large.
THEOREM B’.
Let 03C8 be
an admissible(= non-degenerate) (unitary)
character ontt and let V be a
quasi-large
Harish-Chandra module.Then,
dimWh03C9n,03C8(V)
coincides with the
multiplicity (or
Bernsteindegree) c(V) of V.
For the definition of
c(V),
see[66].
The purpose of this article is to
get
C -00 -counterpart
of this result. In order to describe ourresult,
we introduce several conventions and notations.First, using
the
Killing
form of[go, go],
weidentify
as followsHere,
""’denotes the real
dual, fio
is the Liealgebra
ofN,
and no is theopposite subalgebra
of go. The last inclusion is definedby
the direct sumdecomposition
go =
[go, go] Et)
co, where co is the center of go. The above identification induces inclusionsin’0 ~ i gi z g*. Here,
i is theimaginary
unit.Using
thisinclusion,
weregard
an admissibleunitary (differential) character 03C8
on fi as a element ofig’0
org*.
Anilpotent
G-orbit in go of the maximal dimension( =
2 dimN)
is called aprincipal nilpotent
G-orbit. We denoteby Pr0(G)
the set ofprincipal nilpotent
G-orbits. A
unitary character 03C8
on tt is admissible if andonly
ifi-1 Ad(G)03C8 ~ g*o ~
go is aprincipal nilpotent
G-orbit.Fix an irreducible Harish-Chandra module V and denote
by
I the annihilator of V in the universalenveloping algebra U(g)
of g. The associatedvariety Ass(U(g)/I)
is a closed conicsubvariety
ofg* (for example,
see[68]).
Thecondition
Dim(V)
= dimN (i.e.
V isquasi-large)
isequivalent
to the conditionthat 03C8~Ass(U(g)/I).
For C-~situation,
the condition forWh~n,03C8(V)~0
isdescribed in terms of wave front set
WF(V) of V,
which are studiedby [17], [1, 2, 3] (also
see[26]).
As isexplained
in[17]
or[1],
the associatedvariety
Ass(U(g)/I)
of the annihilator I can beregarded
as thecomplexification
ofWF(V)
and the wave front set
WF(V)
contains moreprecise
information of V thanAss(U(g)/I). (For example,
theholomorphic
and theanti-holomorphic
discreteseries of
SL(2, R)
aredistinguished by
the wave front sets butthey
have the sameassociated varieties of the
annihilators.)
Theprecise
definition of the wave front set of a Harish-Chandra module in this article is discussed in 3.1.Here,
we definethe wave front set as a closed conic subset in
ig’0.
The main theorem of this article is:
THEOREM A
(Theorem 3.3.3).
Let G be a real reductive linear Lie group.Let
be an admissible
unitary
character on fi and let V be a Harish-Chandra(g, K)-
module.
Then,
we haveWh0n,03C8(V) 0 if and only if 03C8
EWF(V).
For
quasi-split
groups, this resultgives
a refinement of[36]
Theorem L. We remark that the above Theorem A for aquasi-split
group withonly
oneprincipal nilpotent
G-orbit isimmediately
deduced from this result of Kostant.About the dimension of
Wh~n,03C8(V),
forquasi-split
groups, the famousmultip- licity
one theorem tells us the dimension ofWh~n,03C8(V)
is one or zero.(This multiplicity
one theorem has along history
and studiedby
many mathemat-icians
[19], [63], [36], [76],
etc. Theversion,
forgeneral
real reductive linear Lie groups, described here is due to Wallach([72]).
Contrary
toquasi-split
groups, it is known that themultiplicity
one theoremfails for
non-quasi-split
groups. Thecounterpart
of Theorem B’ is:THEOREM B
(Theorem 5.5.2).
Let G be a connected real reductive linear Lie group and let V be an irreducible Harish-Chandra(g, K)-module. Let 03C8
be anadmissible
unitary
character on fi suchthat 03C8
EWF(V). Then,
there exists aninteger s
such that1 2s
card3+o(G)
whichonly depends
on V such thatMoreover, if
V is the Harish-Chandra moduleof
a discrete seriesrepresentation,
then 2sequals
card-0,Pr,(G).
We also relate the dimension of the space of Whittaker vectors to the
asymptotic expansion
of the distribution character in the sense of[1].
THEOREM C
(Theorem 5.5.1).
For each OEf!ho(G), we fix
an admissibleunitary
character
t/J (!)
E iO. Let V be aquasi-large
Harish-Chandra module and let03B8V
be thelift of
the distribution characterof
V to go. Then the Fouriertransform of the first
term
of
theasymptotic expansion (cf. [1]) of 03B8V
isHere, 03BCO is
the G-invariant measure on O with a suitable normalization(see §5).
Our
proof of the
above results consists of threesteps. First,
we prove them for real reductive linear Lie groups withonly
oneprincipal nilpotent
orbitusing
asimilar method to that in
[48].
Forsimplicity,
we consider theintegral
infinitesimal character situation. We fix a Cartan
subalgebra 4
and let W be theWeyl
group for(g, 1)).
We denoteby
H thecategory
of Harish-Chandra modules with some fixedregular integral
infinitesimal character(say 03BB)
and denoteby KC(H)
thecomplexified
Grothendieck group of H.Then, Kc(/)
has astructure of W-module via coherent continuations. From a result of
Casselman,
the functor
Wh~n,03C8
is an exact functor from --Y to thecategory
of vector spaces.By
a result ofVogan, dimwhg, (resp.
themultiplicities)
induces a W-homomorphism 03A8 (resp. 03A8’)
fromKC(H)
toS(*).
Put k = cardA + - dim
fi.Then,
we seeImage 03A6~~ikSi(*).
It holds that an irreducible W-module 6 appears as acomposition
factor of bothKC(H)
and~ikSi(*),
then 6 mustcoincide with the
Springer representation
03C30corresponding
to the com-plexification
of theprincipal G-nilpotent
orbit in go. If wedecompose Kc(e)
into the direct sum of blocks
([67, 69],
then we see 6o appears in each block ofKc(/)
and in~ikSi(*)
withmultiplicity
one under theassumption
that Ghas
only
oneprincipal nilpotent
orbit. Thisimplies
that (D and (D’ areproportional
on each block. Theproportionality
constants areeasily
obtainedby comparing dim Wh~n,03C8
and themultiplicities
forprincipal
series represen- tations. Fromthis,
we have 03A6 is non-trivial andproportional
to 03A6’. The mainresults for G with
only
oneprincipal nilpotent
orbit follow from this.The second
step
is to prove the main results for discrete seriesrepresentations.
Besides the conclusion of the first
step,
the mainingredients
of thisstep
are:(1)
Theorem A holds forSL(2, R).
(2)
Schmid’s characteridentity.
(3)
WF andWhg,
well-behave under inductions.(4)
Fine structures ofprincipal nilpotent
orbits described in Section 2.Finally,
we derive the main results in thegeneral
situationusing
the above(3)
and
(4)
from the conclusions ofsteps
1 and 2 and the fact that every irreducible Harish-Chandra module is realized as aLanglands quotient.
The
plan
of this article is as follows. In Section 1 we fix notations. In Section 2we
investigate principal nilpotent
G-orbits. In Section 3 we discuss the definition andproperties
of wave front sets and formulate the main result. In Section 4 weprove the above Theorem A for real reductive linear Lie groups with
only
oneprincipal nilpotent
orbit. In Section5,
we prove the main theorem for thegeneral
case.List of
symbols
1. Notations and
preliminaries
1.1. General notation
In this
article,
we use thefollowing
notations.As usual we denote the
complex
numberfield,
the real numberfield,
the rational numberfield,
thering of integers,
and the set ofnon-negative integers by C, R, Q, Z,
and Nrespectively.
For each setA,
we denoteby
card A thecardinality
of A. We denote theimaginary
unit-1 by
i.For a
complex
vectorspace V,
we denoteby
V* the dual vector space and we denoteby S( V) (resp. Sn(V))
thesymmetric algebra (resp.
the nthsymmetric power)
of E For a real vector spaceV0,
we denoteby V’0
the real dual vector space ofV0. Sometimes,
weidentify S(V)
and thepolynomial ring
over V*. Forany
subspace W
ofV, put W~={f~V*|f|W ~ 0).
Unless wespecify, "(8)"
means the tensor
product
over C.For a real
analytic
manifold X and a Fréchetspace Y,
we denoteby C°°(X) (resp. C’(X, V))
the space of the C-valued(resp. V-valued)
C~-functions on X and denoteby
T*X thecotangent
bundle of X. We denoteby
J.l2 the(multiplicative) cyclic
group of order 2. For any groupQ,
we denoteby Z(Q)
thecenter of
Q.
We denoteby 0
theempty
set. For a set A whose elements are also sets, we define the unionU A by
We denote
by
A - B the set theoretical difference of A from B.For an Abelian
category A,
we denoteby K(.9I)
the Grothendieck group 0 f -ç/.1.2. Notation
for
reductive Lie groups andalgebras
Hereafter we fix a
complex
reductive Liealgebra
g and its real form go. Let co(resp. c)
be the centerof go (resp. g).
We denoteby GadC
theadjoint
groupof g,
so itis a connected
complex semisimple
Lie group. For an Lie groupQ
with the Liealgebra
q, we denoteby Adq (resp. adq)
theadjoint
action ofQ (resp. q)
on q. Forsimplicity,
we denoteby
Ad(resp. ad)
theadjoint
action ofGadC (resp. g)
on g. PutG# = {g
EGal |Ad(g)g0 ~ gol.
We denoteby Gb
theanalytic subgroup
ofGe
withrespect
to[go, go].
Hereafter,
werepresent by
* the one of # or b.We fix an involution 0 of go such that its restriction to
[go, go]
is a Cartaninvolution. We denote the
complexification
0 on g(resp. lifting
toGadC) by
thesame letter. Let go =
10
+ 0(resp.
g = t +e)
be the ±1-eigenspace decomposition
with
respect
to 0. We denoteby
K* the maximalcompact subgroup
of G*corresponding
to10. So, K’
is theidentity
connectedcomponent
ofKe.
PutK#C = {g
EGad 10(g)
=gl
and denoteby KbC
theidentity
connectedcomponent
ofK#C. (In [37], K#C (resp. KbC)
is denotedby Ke (resp. K).)
We fix anon-degenerate
real-valued bilinear
form ,>
on go which satisfies thefollowing.
(Bl) ,>
ispositive
definite(resp. negative definite)
on 50(resp. to).
(B2)
The restrictionsof ,>
to[go, go]
coincides with theKilling
form of[go, g0].
Clearly,
such a bilinear form exists and we also denote thecomplexification
of,> by
the same letter.We fix a maximal abelian
subspace sa0
in s0 and denoteby smo
the centerizer ofsa0
into.
We also fix a Cartansubalgebra sto
ofsm0.
We
put
Here,
exp is theexponential
map of[g, g]
toGadC.
LEMMA 1.2.1
([37], [42]). Fe
coincides with the groupof
order two elements inexpea)
andFe
normalizesGb, Kb,
andKbC. Moreover,
we haveG# = GbF#, K#C
=KbCF#,
andK#
=KbF#.
Put
-’40 =Sto +sao. Then, Sho
is a(maximally split)
Cartansubalgebra
of go. We fix aparabolic subalgebra spo of go
whose Levipart
issmo + sao. spo is
a minimalparabolic subalgebra
of go.Let no be the nilradical of
Spo
and letno
be theopposite nilpotent subalgebra
to n0, so we have go = no +
smo
+Sao
+tto.
We denote thecomplexifications
ofsao, SMOI stol S40, spo, ... by sa, sm, S t, sb, Sp, ... , respectively.
We call goquasi- split,
if’p
is a Borelsubalgebra
of g.Let A be the root
system
withrespect
to(g, sh).
We fix apositive
rootsystem 0394+ compatible
with n, and denoteby
II the set ofsimple
rootsin A +.
Let W bethe
Weyl
group of thepair (g, sh)
and we denote the innerproduct
onsh*
whichis induced
from (, ) by
the same letter. For a~0394,
we denoteby
sa the reflection withrespect
to a. We denoteby
wo thelongest
element of WFor a
EA,
we define the corootby
â =2a .
We call 03BB~ sh*
dominant(resp.
antidominant),
if03BB, >
is not anegative (resp. positive) integer,
for each03B1 ~ 0394+.
We
call 03BB~sh* regular,
if03BB, 03B1> ~ 0,
for each 03B1 ~ 0394. We denoteby
Q the space of Z-linear span of the roots. We denoteby
P theintegral weight lattice, namely
P
= {03BB ~ sh* 1 (Â, >
e Z forall 03B1 ~ 0394}. If 03BB ~ sh*
is contained inP,
we call 03BBintegral.
Let
P - -, P -, P + +,
andP +
be the space of antidominantregular integral weights,
antidominantintegral weights,
dominantregular integral weights,
anddominant
integral weights, respectively.
For
regular 03BC~sh*,
we defineintegral
rootsystem 039403BC by
Put
0394+03BC=039403BC~0394+,
then it is apositive system of LlJl.
We denoteby rl,
thesimple
root
system of 0394+03BC.
We also define theintegral Weyl
groupby
It is known that
W03BC
is theWeyl
group for the rootsystem 039403BC.
We define
pEsl)* by
p= 1 203A303B1~0394+03B1.
As axioms for real reductive linear Lie groups, we choose here those in
[67]
p. 1.
Namely,
we say that aquadruplet (G, g0, 03B8, ,>)
is a real reductive linear Liegroup, if it satisfies the
following
conditions.(Often,
wesimply
say G is a real reductive linear Liegroup.)
(RL1)
G is a real Lie group and the Liealgebra
of G is go.(RL2) GD ç; Ad(G) z G’.
(RL3)
There is an maximalcompact subgroup
K of G such that the Liealgebra
of K isto
and K xexp(s0) ~
Gby (k, X) ---> k exp(X) (k
EK,
X Es0),
whereexp is the
exponential
map of go to G.(RL4)
There is a faithful finite-dimensional linearrepresentation
of G.(RL5)
Letho
be anarbitrary
Cartansubalgebra
of go. Let H be the centerizer of1)0
in G.Then, H
is abelian.Moreover,
if go issemisimple (resp. simple),
we call G a realsemisimple (resp.
simple)
linear Lie group.A real reductive linear Lie group is a real Lie group of matrices in the sense of
[30]. Hence,
we canapply Knapp-Zuckerman theory ([33])
fortempered representations
to real reductive linear Lie groups.Hereafter,
we fix a real reductive linear Lie group G as above.Let
SA, N,
andN
be theanalytic subgroup
in G withrespect
tosa0,
no, andtto, respectively.
We denoteby
SM(resp. S T)
the centerizerof Sao (resp. ’40) in K
withrespect
to theadjoint
action. Put SP = SMSAN. Then sP is a minimalparabolic subgroup
of G. LetS To
be theidentity component
of sr.Next we fix the notations on the restricted root
system.
Wealways regard
Sa*as a
subspace
ofsl)* by
the zero extension to fi. Since the Cartan involution 0acts on
Sh,
it also acts on A.Following [67],
we introduce thefollowing
notions.We call a root a e A real
(resp. imaginary)
if a= -03B8(03B1) (resp.
a =03B8(03B1)).
We call03B1~0394
complex
if a is neither real norcomplex.
Letllreal, 5 Ilimaginary and rleomplex
be the set of
real, imaginary,
andcomplex simple
roots,respectively.
Let 1 be the set of restricted roots with
respect
to(go, Sao),
and letE +
be thepositive system
of 1compatible
to0394+. Namely, 03B2=03B1|sa
forsome
a c- AI.
Let 0 be the set ofsimple
restricted roots in03A3+.
Weidentify
realroots and
corresponding
restricted roots.So,
we haveHere, (Dreal
=1 Ireal
and03A6complex = {1 2(03B1 - 0(’X» 1
a E03A0complex}.
For a~ 03A3,
we denoteby go,a the
root space in go withrespect
to a.For
03B1 ~ 03A6,
we denoteby H03B1
the element insa0
n[go, go]
such that03BB(H03B1) = 03BB, 03B1>
for all A E sa*.For a
~ 03A6,
we denoteby 03A903B1
the element inlao
n[go, go]
such that03B1(03A903B1)
= 1 and03B2(03A903B1)=0
for all03B2 ~ 03A6 - {03B1}.
Let W(X =exp(03C0i03A903B1)
for a E03A6,
where exp is theexponential
map of[g, g]
toG al. Clearly,
we haveW2
= 1 and 03C903B1 EFe. Here,
1 is theidentity
element.Moreover,
we caneasily
see(cf. [55]
p.406) Fe
isgenerated by {03C903B1|03B1~03A6}.
1.3. Fine structures
of parabolic subgroups
Let G be a real reductive linear Lie group and let sP
(resp. SH)
be the minimalparabolic (resp. maximally split Cartan) subgroup
withrespect
toSpo (resp. sbo), namely
SP is the normalizer(resp. centerizer)
of’p, (resp. bo)
in G.Hence,
wehave SH = STSA. A
parabolic subgroup
P of G(resp.
aparabolic subalgebra po
ofgo)
is called standard if P ~ sP(resp.
Po ;2Spo).
We call a Levidecomposition
P = LU
(resp.
po =10
+uo) standard,
if sH ~; L(resp. sh0 ~ I0).
It is known that L is also a real reductive linear Lie group. We denoteby Lb (resp. Lo)
theidentity
connected
component
ofAdj(L) (resp. L).
We say that a standard
parabolic subgroup
P(resp. subalgebra po)
iscorresponding
to 5’ c C if S is asimple
restricted rootsystem
for(10, 1)0).
It iswell-known that this
correspondence gives
one to onecorrespondence
betweenthe set of standard
parabolic subgroups
and the set of subsets in 03A6.Sometimes,
we
represent
the standardparabolic subalgebra
pocorresponding
to S ~ 03A6 asfollows.
Namely,
wereplace "0" by "0"
at the vertices of theDynkin diagram
of 03A6
corresponding
the elements of SWe denote
by Go
theidentity component
of G and denoteby Gc
thecomplexification
ofGo.
For03B1 ~ 03A6,
weput h03B1 = exp(03C0iH03B1)~G. Here,
exp is theexponential
map of g toGc.
Weput ha
=Ad(ha).
We denoteby FG (resp. Fb)
thegroup
generated by {h03B1|03B1~03A6} (resp. {h03B1|03B1~03A6}). So, Fb = Ad(F0G). Clearly
Fb ~ F#.
We caneasily
seeh03B1 ~ K
nGo
andha
EKb.
For
51(2, R),
we fix a Cartan involution 0 such that0(2)
is the +1-eigenspace
for0.
For a in
03A6real,
there is a Liealgebra homomorphism fa of I(2, R)
to go such thatWe can
(and do)
assume that 0 -f03B1 = f03B1°
03B8. For a in03A6real, fa
is liftable to a grouphomomorphism ~03B1
ofSL(2, R)
toGo
such thatPut
Fa
=Ad-1(Ad(K)
nexpea
n[g, g])). Here,
exp means theexponential
map of
[g, g]
toGadC.
The
following
is known.LEMMA 1.3.1
(cf. [75]
Lemma1.2.4.5, [42]).
Let G be a real reductive linear Lie group, let P be a standardparabolic subgroup of G,
and let P = LU be the standard Levidecomposition of P. Then,
we have L =LoFG.
We denote
by
C theanalytic subgroup
of Gcorresponding
to Co. Thefollowing
lemmaeasily
follows from the factZ(G) ~
KC.LEMMA 1.3.2
(cf. [33] p.400).
We assumeG, P,
and L is as in Lemma 1.3.1.Moreover,
we assume G is connected. ThenFG
=Z(G)FG
andAd(FG)
=Fb.
For a e
03A6,
we defineThen,
weeasily
have:LEMMA 1.3.3. We assume that g does not have a
G2-type.factor. Then, for
a E03A6],
1.4. Notations
for
Harish-Chandra modulesWe denote
by U(g)
the universalenveloping algebra
of g andby Z(g)
the centerof
U(g).
For 03BB~sh*,
let x;.:Z(g) ~ C
be the Harish-Chandrahomomorphism.
Weparametrize
them sothat X,
= Xw;’ for all w E W We say aU(g)-module V
has aninfinitesimal
character ~03BB
iffZ(g)
acts on Vthrough
XÂ.For a real reductive linear Lie group
(G, g0, 03B8, , >).
We denoteby HG (resp.
eG [Â])
thecategory
of Harish-Chandra(g, K)-modules (resp.
Harish-Chandra(g, K)-modules
such that all the irreducible constituents have agiven
in-finitesimal character
/J.
2.
Principal nilpotent
orbits2.1.
Principal nilpotent
orbitsAs in Section
1,
let g be acomplex
reductive Liealgebra
and let go be a real formof g.
First,
we define thenilpotent
cone as usualby
We call an element of X a
nilpotent
element in g. Then aV’ is a closed conicalgebraic variety
of dimension card A. AGadC-orbit
of g under theadjoint
actionis called a
nilpotent
orbit if it is contained in X.Similarly,
a G*-orbit(resp. Kt- orbit)
of go(resp. )
under theadjoint
action is called anilpotent
orbit if it is contained in X n go(resp.
X n5). Here,
G*(resp. Kt)
means anarbitrary
group such that
GIJ £;
G* zGe (resp. KbC ~ K*C ~ K#C).
A
nilpotent
orbit of maximal dimension calledprincipal ([34, 35], [37], [54], etc.).
The number of the
principal GadC-, K#C-,
orG#-nilpotent
orbits isjust
one, butthe number of
principal nilpotent Gb-
orKbC-orbits
need not be one([34, 35], [37], [55]).
Inparticular,
we denote theunique principal nilpotent GadC-, G#-,
andK#C-orbit by mëg, (9e ,
and(9e, respectively.
We call an element in(9"g
aregular nilpotent
element. We havemëg n g0 ~ 0 (resp. (9"g ~~Ø)
if andonly
if go isquasi-split.
If go isquasi-split,
then we havemëg n
go =(9e
and(9"g
n 5 =(9e
Since there is a natural
(up
toparity) bijection
between the set ofprincipal nilpotent Gb-orbits
and that ofprincipal nilpotent KbC-orbits ([55]),
the numberof
principal nilpotent Gb-orbits
coincides with that ofprincipal nilpotent KbC-
orbits.
We denote
by
F’ thesubgroup of Fe generated by {03C903B1 a
E4) complexl-
We denote
by c(go)
the number ofprincipal nilpotent Gb-orbits
in go. Thefollowing
result is known.LEMMA 2.1.1
([61]). (A)
Let go be a realquasi-split simple
Liealgebra.
Then thenumber
of principal nilpotent KbC-orbits
in 5(so,
it coincides withc(g0))
is oneexcept the
following
cases(l)-(9).
(2)
go =sp(2n, R) (n 2): c(90) =
2.(3)
go =so(2n + 1, 2n + 1) (n 2): c(go)
= 2.(4)
go =50(2n, 2n) (n 2): c(go)
= 4.(5)
go =so(2n + 1, 2n) (n 2): c(go)
= 2.(6)
go =so(2n
+2,
2n +1) (n 1): c(90) =
2.(7)
go = a normalreal form of
e7 :c(go)
= 2.(8)
go =su(n, n) (n 2): c(go)
= 2.(9)
go =so(2n
+2, 2n) (n 2) : c(go)
= 2.(Here,
the real rankof sp(2n, R)
is n.51(2, R) belongs
to(1).)
(B)
Let go be a realnon-quasi-split simple
Liealgebra.
Then the numberof principal nilpotent KbC-orbits
in s(so,
it coincides withc(g0))
is one except thefollowing
cases(10)-(12).
In each case(10)-(12), c(go)
= 2.(10)
go =50*(4n) (n 3).
(11)
go =so(2n+k, 2n) (n 1, k 3).
(12)
go = areal form of
e7 associated to an Hermitiansymmetric
space,namely
the EVII type.
For the relation of
c(go)
toFe, Fb,
andFc,
thefollowing
is known.LEMMA 2.1.2
([55]
Theorem4.6, 5.3). (1)
For03C3 ~ Fc, we
haveAd(a)(9
=O for
allprincipal nilpotent GD -orbit
(9.If
go isquasi-split,
then Fc ~Fb.
(2)
Let O be aprincipal nilpotent GD -orbit
in go and let{n1,..., nkl
be the setof representative
inF# for
thequotient
groupF#/FbFc. Then, {Ad(n1)O, ..., Ad(nk)O}
is a
complete
setof
the distinctGD -principal nilpotent
orbits in go. Inparticular
card(F#/FbFc)
=c(go).
Using
Lemma1.3.3,
we can describeF#, Fb,
and Fc for(1)-(12)
in Lemma2.1.1,
as follows. Information on restricted roots is found in
[75]
p. 30-32.(1)
go =I(2n, R) (n 1).
In this case, Fc is trivial and
hy
is non-trivial for any y E 03A6. We fix a numeration 03B11,..., 03B12n-1 of 03A6 suchthat 03B1i, 03B1i+1> = -1
for all 1 i 2n - 2.Then,
wehave:
(la) Wai E FD
if andonly
if i is even.(lb) F’ = F’
uwaiFD
for any odd i.(2)
go =sp(2n, R) (n 2)
In this case, Fc is trivial and
hy
is non-trivial for any y E 03A6. Let a be thelong simple
root. Let03B21, ... , 03B2n-1
be the numeration of shortsimple
roots such that03B2i,03B2i+1>= -1
for all 1 i n - 2 and03B2n-1,03B1> = -1. Then,
we have:(2a) úJPi E FD
for all 1 i n - 1 and03C903B1 ~ Fb.
(2b) F’ = Fb ~ waFD.
(3) S0=S0(2n+1, 2n+1) (n 2)
In this case, F’ is trivial and
hy
is non-trivial for any03B3 ~ 03A6.
Let03B21, ..., P2, - 1,
a 1, a2 be the numeration of
simple
roots such that03B2i,03B2i+1>=-1
for all1 i 2n - 2 and
03B22n-1, 03B1i> = - 1
for i= 1, 2. Then,
we have:(3a) 03C903B2i ~ Fb
for all 1 i 2n -1 and03C903B1i ~ Fb
for i =1, 2.
(3b) F’ = Fb ~ 03C903B1iFb
for i =1, 2.
(4)
go =sb(2n, 2n) (n 2)
In this case, F’ is trivial
and hy
is non-trivial for any03B3 ~ 03A6.
Let03B21, ..., P2n -
2,al, a2 be the numeration of
simple
restricted roots such that03B2i, 03B2i+1>
= -1 forall 1 i 2n - 3 and
03B22n- 2, 03B1i>
= -1 for i =1, 2. Then,
we have:(4a)
WPiE Fb
if andonly
if i is even.Moreover, 03C903B1i ~ Fb
for i =1, 2.
(4b)
In this caseF#/Fb
isisomorphic
to 03BC2 03BC2. For any odd1 i 2n - 2,
we have
In this case, F’ is trivial
and ha
is non-trivial for anylong simple
restricted root 03B1 ~ 03A6.Let fi
be aunique
shortsimple
root in 03A6.Then, h03B2 = 1.
We fix anumeration al, ... , a2n -1
of long simple
roots in 03A6 such that03B1i, 03B1i+1>
= -1 forall 1 i 2n - 2 and
(a2n-l, 03B2> = -2. Then,
we have:(5a)
03C903B1i eFb
if andonly
if i is even.Moreover,
wp eFI:J.
(5b) F’ = F’
u03C903B1iFb
for all odd 1 i 2n -1.(6)
90 =sb(2n + 2, 2n + 1) (n 1)
In this case, F’ is trivial
and ha
is non-trivial for anylong simple
restricted root 03B1 ~ 03A6. Letfi
be aunique
shortsimple
root in 03A6.Then, h03B2 = 1.
We fix anumeration a,, ... , a2n
of long simple
roots in 03A6 such that(ai’ 03B1i+1>
= -1 for all1 i 2n -1 and
(a2n, 03B2> = -2. Then,
we have:(6a)
cvai EFb
if andonly
if i is even.Moreover, 03C903B2 ~ Fb.
(6b) F#
=Fl:JuwaiFP
for all odd 1 i 2n-1 andF#
=Fb ~ 03C903B2Fb.
(7)
go = a normal real form of e7In this case, F’ is trivial
and h03B1
is non-trivial for anysimple
restricted root a E 03A6.We fix a numeration ai , ... , a7 of
simple
roots in 03A6 such that03B1i, 03B1i+1>
= -1 forall 1 i 5 and
03B14, 03B17> = - 1. Then,
we have:(7a)
c-F5
if andonly
if i =2, 4, 5,
6.(7b) F#
=Fb ~ 03C903B1iFb
for i =1, 3,
7.In this case,
ho
is non-trivial for allsimple
restricted root03B2.
Let a be aunique
realsimple
restricted root in 03A6. We fix a numeration 03B31, ..., 03B3n-1 ofcomplex simple
roots in 03A6 such that
03B3i, 03B3i+1> = -1
for all 1 i n - 2 and03B3n-1, 03B1>= -1.
Then we have:
Let y be a
unique complex simple
restricted root in 03A6. We fix a numeration 03B11,..., a2n - 1 oflong simple
real roots in 03A6 such that03B1i, 03B1i+1>
= -1 for all1 i 2n - 2
and03B12n, 03B3> = -2.
In this caseh03B3 = 1 and h03B1i ~ 1
for1 i 2n -1.
Moreover,
we have:In this case
h03B3
=1 1 for all y ~ 03A6. Let oc be thelong simple
restricted root. Let03B21,...,03B2n-1
be the numeration of shortsimple
restricted roots such that03B2i, 03B2i+1> = - 1
for all1 in-2
and03B2n-1, 03B1> = -1.
In this case,03A6complex = {03B21,
...,03B2n-1}. Moreover,
we have:Let y be a
unique complex simple
restricted root in 03A6. We fix a numeration 03B11, ...,a2n - 1 of long simple
real restricted roots in 03A6 such that03B1i, 03B1i+1>
= -1for all 1 i 2n - 2 and
03B12n,03B3>=-2.
In this casehy =1 and h03B1i ~
1 for1 i 2n -1.
Moreover,
we have:(12)
go = a real formof e7
associated to an Hermitiansymmetric
space,namely
the EVII
type
In this case
hy =1
1 for all03B3 ~ 03A6.
Let a be thelong simple
restricted root. Let03B21
and
03B22
be the numeration of the shortsimple
restricted roots such that03B21, 03B22> = -1
and03B22, 03B1> = -1.
In this case,03A6complex
={03B21, fi2j. Moreover,
wehave:
Finally,
we remark:LEMMA 2.1.3. Let go be a
simple
real Liealgebra
which is oneof (l)-(12)
inLemma 2.1.1. Then we have:
(1)
The restricted root system 03A3 is reduced.(2)
Fc -F’.
(3) Any long simple
restricted root is real.2.2.
Principal nilpotent
orbitsfor
Levisubgroups
Let go be a
simple
real Liealgebra
which is oneof (1)-(12)
in Lemma 2.1.1. In this case, weput S0 = {03B1~03A6|03C903B1~Fb}.
We denoteby po
the standardparabolic subalgebra
of go such thatSo
is thesimple
restricted rootsystem
of the standard Levifactor I0 of p0.
From the abovedescription of Fb, Po
is described as follows.(1)
If go =51(2n, R),
thenPo
is the standardparabolic subalgebra
such that thesemisimple part of10
isisomorphic
to the directproduct
of ncopies
ofsl(2, R).
Namely,
(2)
If go =sp(2n, R),
thenPo
is the standardparabolic subalgebra correspond- ing
to S ={the long simple rooti.
Thesemisimple part
of10
isisomorphic
to51(2, R). Namely,
(3) If go
=so(2n + 1, 2n + 1),
then thesemisimple part of I0
isisomorphic
to thedirect sum of 2
copies
ofsI(2, R). po
is described as follows(4)
If go =so(2n, 2n),
thenPo
is the standardparabolic subgroup
such that thesemisimple part
of10
isisomorphic
to the directproduct
of n + 1copies
of61(2, R). Namely,
(5)
If go =50(2n
+1, 2n),
thenPo
is a standardparabolic subgroup
such thatthe
semisimple part
of10
isisomorphic
to the directproduct
of ncopies
ofsI(2, R).
po isrepresented
as follows(6)
Ifg0 = s0(2n + 2, 2n + 1),
thenPo
is the standardparabolic subgroup
suchthat the
semisimple part of I0
isisomorphic
to the directproduct
of n + 1copies
of
sI(2, R). Namely,
(7)
If go = the normal real form ofE7,
thenPo
isrepresented
as follows(8)
If go =5u(n, n),
thenPo
is aunique
standardparabolic subalgebra
suchthat the
semisimple part ofTo
issI(2, R). Namely,
(9)
If go =so(2n
+2, 2n),
thenPo
is a standardparabolic subalgebra
such thatthe
semisimple part
of10
isisomorphic
to the directproduct
of ncopies
of51(2, R). Namely,
(10) If go
=so*(4n),
thenPo
is the standardparabolic subalgebra correspond- ing
to S ={the long simple root}.
Thesemisimple part of I0
is the directproduct
of one copy of
51(2, R)
and ncopies
ofs0(3). Namely,
(11)
If go =so(2n + k, 2n) (n , 1, k 3),
thenPo
is a standardparabolic subalgebra
such that thesemisimple part
ofÎo
isisomorphic
to the directproduct
of ncopies
of51(2, R)
and one copy of5-,o(k). Namely,
(12)
If go = a real form of e7 associated to an Hermitiansymmetric
space,then
Po
is the standardparabolic subalgebra corresponding
to S ={the long simple root}.
Thesemisimple part
of10
issI(2, R)
x50(8). Namely,
Now,
we assume go =so(2n, 2n)
and G is a connectedsimple
real linear Lie group whose Liealgebra
is go. We definesubgroups Fi (i
=1, 2, 3)
ofFe
asfollows
Fi
isgenerated by {03C903B2i| 1
is odd and 1 i 2n -2},
F2
isgenerated by {03C903B11}, F3
isgenerated by {03C903B12}.
For i =
1, 2, 3,
weput Si = {03B1 ~ 03A6|03C903B1 ~ FbFi}.
LetPi
be the standardparabolic
subalgebra
of go =so(2n, 2n) corresponding
toSi.
These arerepresented
asfollows.
Fix real reductive linear Lie group G and a
parabolic subgroup
P with thestandard Levi
decomposition
P = L U. We denoteby c(L) (resp. c(G))
the numberof
principal nilpotent
L-orbits in10 (resp.
G-orbits ingo). P
is calledtype
1(resp.
type II),
ifc(L)
> 1(resp. c(L)
=1).
Inparticular,
we say G is oftype
1(resp.
type II)
if there exists more than one(resp. exists just one) principal nilpotent
G-orbits
(resp. G-orbit)
in go. Lemma 2.1.1 tells us which connected realsimple
Liegroup is
type
I. Forparabolic subgroups,
we have:LEMMA 2.2.1.