C OMPOSITIO M ATHEMATICA
S. R ALLIS
On the howe duality conjecture
Compositio Mathematica, tome 51, n
o3 (1984), p. 333-399
<http://www.numdam.org/item?id=CM_1984__51_3_333_0>
© Foundation Compositio Mathematica, 1984, tous droits réservés.
L’accès aux archives de la revue « Compositio Mathematica » (http:
//http://www.compositio.nl/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
333
ON THE HOWE DUALITY CONJECTURE
S. Rallis
© 1984 Martinus Nijhoff Publishers, The Hague. Printed in The Netherlands
Table of contents
Introduction
The purpose of this paper is to establish certain results in the
theory
ofcusp forms for the classical groups of the
type Sp,,
orO( Q ) (symplectic
and
orthogonal).
Thetheory
forGtn
has been initiated and iscontinuing
to be
developed,
thanksmainly
to the efforts ofHecke, Godement, Jacquet, Langlands, Piatetski-Shapiro,
and Shalika. There areessentially
two main
problems
in theGt:l
case.First,
it is necessary todevelop
aHecke
theory
forautomorphic cuspidal representations
ofGtn.
Thatis, using
the L-functiontheory
of admissibleGtn(A) representations given
in
[J-Ps-Sh]
and[G-J],
one wants to characterize theautomorphic cuspidal representation
in terms of theholomorphicity
of the associated L-func- tion and thefamily
of functionalequations
that the "twists" of the L-functions mustsatisfy.
The secondquestion
is to follow thegeneral Langlands philosophy
and determine whether such L-functions can beinterpreted
asArtin-type L-functions, i.e.,
L-functions associated to finite dimensionalrepresentations
of certainWeil-Deligne
groups. On the otherhand,
to answer similarquestions
forSp,,
orO(Q)
seems to be at a veryrudimentary stage. Indeed,
very recent progress has beengiven
in[Ps-1]
to
develop
asystematic theory
of L-functions forSp2.
What is evidentThis research was supported, in part, by NSF Grant MCS 78-02414.
from the various
empirical
observations in[H-Ps-1]
and[Ps-2]
is severalphenomena
that do not occur in theGê,
case.Namely (1)
L-functions ofcuspidal representations
may havepoles
and(2) "Ramanujan"
typeconjectures fail;
thatis, eigenvalues
of Heckeoperators operating
on cusp forms fail to be"unitary"
ortempered
in certain directions. Thesespecific phenomena
are, infact,
veryintimately connected; they
comefrom
using lifting theory
associated to Weilrepresentations
of dualreductive
pairs.
Thus our purpose here is to use
lifting theory
togive
adecomposition
of the space of cusp forms on these groups into
orthogonal "pieces" R,,
where all the irreducible
components occurring
inR, (for
certaini)
exhibit the
specific phenomena
indicated above. Thekey point
here is toshow that such a
lifting theory
canactually
be formulated inprecise
terms
(see [H]).
Thatis,
for eachsubspace R,,
werequire
that there is awell defined
mapping
fromautomorphic representations occurring
inR,
to
cuspidal automorphic representations
on some other groupG,.
More-over we want that such a
mapping
beinjective
and preserve themultiplic-
ities of the
representations.
One additional
point
thatinevitably
comes with such aninvestigation
is how to use the
Selberg
Trace Formula to get an effective"comparison
of traces" statement between Hecke
operators
on the various groups involved in thelifting. Specifically
we present belowpreliminary
evidencethat such a
comparison
of trace ispossible;
the maindeparture
from theclassical cases is that we
require comparison
of traces for notjust
onefixed dual
pair
but for a wholefamily
of dualpairs!
Indeed we start with a fixed
orthogonal
groupO( Q ) (where Q
isdefined on an m dimensional
space)
and consider the space of cusp formsL2cusp(O(Q)(A))
onO(Q)(K)BO(Q)(A).
Then we define for eachf
inL2cusp
the "lift"of f as
the span of functionswhere Orp
is a 03B8-series on the groupSpn(A)
XO(Q)(A)
constructed from the associated Weilrepresentation
of the dual reductivepair (Spn, O(Q)) (where ~
varies over all Schwartz-Bruhatfunctions).
Then for eachirreducible
component (77-)
inL2cusp,
welet An(03C0)
= the space of the "lift"of f as f varies
in(03C0).
Then the firstpoint
we show is that(1)
Thespace An(03C0) ~ L2cusp(Spn(A)) ~
theliftj Ar(03C0)
of 03C0 isidentically
zero for all
1
r n - 1.This rather
elementary
criterion then allows us to determine a naturaldecomposition (Theorem 1.2.1)
of the spaceL2cusp
into anorthogonal
directsum of
O(Q)(A)
invariantsubspaces
where a
representation
qroccurring
inR has
theimportant property
thatthe
representation
will die under"lifting"
toSpr(A)
when r t, and r = tis the first
positive
number where 03C0 lifts to a nonzerocuspidal
representa- tion inL2cusp(Spt(A)).
It mayhappen
that qr will lift to a nonzerocuspidal
representation
inL2cusp(Spt(A))
for t > r. This then leadsnaturally
to theglobal
Howeduality conjecture (see [H])
which states that(*) given
acuspidal representation
qroccurring
inR,,
then there is aunique cuspidal representation 03B2l(03C0) occurring
inL2cusp(Spl(A))
suchthat Al(03C0) ~ L2cusp(Spl (A))
is a nonzeromultiple
offil (03C0).
Moreoverthe induced
mapping
is an
injective mapping
from the set ofrepresentations
ofO(Q)(A) occurring
inR,
into the set ofcuspidal representations
ofSpi(A).
The
import
of theconjecture
is that thelifting
defined betweenR,
andL2cusp(Spl(A)) gives,
infact,
awell-defined mapping
betweenrepresenta-
tions which isinjective!
We then show that the
global duality conjecture
isimplied by
the localduality conjecture (Theorem 1.2.2) for
allprimes
v in K. Inparticular,
thelocal
duality conjecture
is a statement about local Weilrepresentations
ofO(Ql’) X Spn(K,,); namely
ifHomO(Qt) Spn(K)(S[Mmn(Ku)], 03C9~03C31) ~ 0,
then 03C31 ~ 03C32
(Spn(Kv) equivalent),
and ifHomO(Ql) Spn(Kl) (S[Mmn(Kv)], 03C91~03C3) ~ 0,
then 03C91 ~ 03C92(O(Qv) equivalent). Here w,
03C91, w2, and a, ul, and a2 are all unitarizablerepresentations.
The mainsubject
in this paper is then to indicate how the localduality conjecture
can be
proved
in various cases;namely,
if(i) Qv
isanisotropic (already
done in[As], [K-V],
and[H]), (ii) Qv
is anarbitrary
form with v finite and dimQv
> 4n +2, (iii) Q,
is anonquaternionic
form with v finite and dimQ,,
= 4n +2, (iv) Qv
is asplit
form with v finite and dimQv
=4n,
(v) Qv
is an unramified form with dimQv n
+ 2.We note here the "almost"
everywhere
statement in[H].
We think that the methodsgiven
below willprobably
extend(with
someeffort)
to allforms
Qv
for each localprime
v.Then
returning
to theglobal
Howeduality conjecture,
it ispossible
torefine the
conjecture by specifying
the behavior ofmultiplicities
underthe map
03B2l given
above. Thatis,
weconjecture
that for each 77occurring
in
R,,
wehave " multiplicity
of qr inR,
=multiplicity
of03B2l(03C0)
inL2cusp(Spl(A))".
Indeed we can show that thismultiplicity preserving conjecture
isimplied by
a localmultiplicity-one conjecture (Corollary
toTheorem
1.2.2)
forall primes
v in K.Again
this is a statement about thelocal Weil
representations
ofO(Q,,)
XSpn(Kv); namely for unitary
repre- sentations m and a, we havedimC(HomO(Qv) Spn(Kc)(S[Mmn(Kv)],
03C9 ~03C3))
1. But then we show that this is true in the cases where we canprove the local
duality conjecture.
Thus we can
actually
show theglobal
Howeduality conjecture
and themultiplicity preserving
statement are valid in certain cases(see
end of1.2).
We note that in
[R-1] we
havegiven
theexplicit
relation between the action of the Heckealgebras
ofO(Q,,)
andSpn(Kv)
in the local Weilrepresentation 77Q,
onS[Mmn(Kv)].
Inparticular, using
thedecomposi-
tion of
L2cusp above,
we canreasonably expect
that there exists acompari-
son of trace formula of the
following
form.If 1:,
is agiven
Hecke operatoron
L2cusp (i.e., fv belongs
to the local Heckealgebra
ofO(Q,,)
at theprime v ),
thenTr(fu)
onL2cusp(O(Q)(A))
has to becompared
with the sumwhere flv
is the Hecke operator onSpl(Kv) paired to 1:, (in
the correspon- dence in[R-1]).
The maindifficulty
here is to have an effective way tocompute Tr(flv|Im 03B2l) using
theSelberg
trace formula.We
organize
the paper in thefollowing
fashion.In
§0
wepresent preliminary
definitions and notation. InChapter
1there are two sections. We are concerned with the
global theory
of cusp forms onO(Q)
orSp.
First in§1
ofChapter I,
we determine(Theorem I.1)
the constant term of the "lift" of a cuspform f(f ~ L2cusp(O(Q)(A)))
along
any maximalparabolic
inSpr(A).
We also determine in an analo- gous fashion the constant term of the "lift" of a cusp formf (for f ~ L2cusp(Spr(A))) along
any maximalparabolic
inO(Q).
Then in§2
ofChapter I,
we deduce thesimple
criterion(Corollary
to Theorem1.1)
stated above for the "lift" to be a cusp form.
Again
we do theanalogous
statement for
Sp,.
Then we define the spacesR,
and show in Theorem 1.2.1 a "finiteness" statement about theR,
and deduce theorthogonal decomposition
ofL2cusp(O(Q)(A))
=~ l=m Rl. Again
we deduce an analo-gous statement for
L2cusp(Spn(A)).
Then we state theglobal
Howeduality
conjecture
and show in Theorem 1.2.2 that thisconjecture
isimplied by
the local
duality conjecture
for allprimes v
in K. In theproof
weintroduce a certain
O(Q)(A)
XSp1(A) invariant,
bilinear nonzero formon the space
S[Mml(A)] ~ 03C0 ~
a(where
03C0, a arecuspidal representations
of
O(Q)
andSp),
which is factorizable into aproduct
of localO(Qv)
XSpl(Kv)
invariantsesquilinear forms;
this allows us to reduce theglobal duality conjecture
to the localduality conjecture
stated above(for
allprimes).
On the otherhand,
weagain
use thisglobal
distribution and its factorizableproperty
to show that(Corollary
to Theorem1.2.2)
localmultiplicity-one implies
theglobal multiplicity preserving
statement.Then we indicate at the end of 1.2 for which cases we can prove the
global duality conjecture.
In
§3
ofChapter I,
we consider thespecial example
of the spaceL2cusp(Sp2(A)).
Inparticular,
there is anorthogonal decomposition
of thisspace into three
subspaces Il(Hl-1)
with i =3, 4, 5,
such thatIl(Hl-1)
lifts to
L2cusp(O(Hl-1)(A))
withH,-,
1 theunique split
form in 2i-2 variables. Then wegive
asimple
criterion for functions tobelong
to thevarious
Il(Hl-1)
in terms of thevanishing
of certain "periods."
We showthat the space
I5(H4)
contains all thoseautomorphic cuspidal representa-
tions without standard Whittaker models. Thus the Saito-Kurokawa space of[Ps-2]
lies inI5(H4);
we show that this latter space does not fill upI5(H4) by giving examples
ofautomorphic cuspidal representations
ofSp2(A)
which are nonzero lifts fromquaternion algebras (see [H-Ps-2]).
The
point
here is that suchexamples satisfy
thegeneralized Ramanujan conjecture
whereas thoserepresentations lying
in the Saito-Kurokawa space do not.Chapter
II is concerned withproving
the localduality conjecture
forthe cases mentioned above.
Indeed here we follow a method of
proof
similar to thatproposed
in[H].
Inparticular,
in 11.1 we prove the "invariant distribution" Theorem(Theorem 11.1).
Thatis,
for any local Weilrepresentation 03C0Qv
ofO(Qv)
XSpn(Kv)
on the spaceS[Mmn(Kv)],
we show that theJacquet
moduleS[Mmn(Kv)]O(Qv)
in the sense of[B-Z]
as anSpn(Kv)
module is isomor-phic
to theSpn(Kv)
module determined as the range of themapping
~ ~
{03C0Qv(G)(~)[0]} (with ~ ~ S[Mmn(Kv)]).
Thus we have a structureTheorem about the space of
O(Qv)
invariant distributions onS[Mmn(Kv)].
Inparticular,
thisgeneralizes
a similar structure Theoremfor the case when n = 1 in
[R-S-1].
We also indicate that ananalogous
statement is true for the
symplectic
case.In 11.2 we consider the restriction of
Sp2n(Kv)
modulePQ,.
=S[Mm2n(Kv)]O(Qv)
to thesubgroup Spn(Kv) Spn(Kv) (embedded
inSp2n(Kv)
via(gl’ g2)
[g1 0]).
We first consider03C1Qv
embedded in abigger SP2n
moduleVm/2,
which is anSP2n
inducedmodule, coming
fromthe
quasi-character
on the maximalparabolic P2 n
0394(Qv) = the
discriminant ofQu.
Then(using
theanalogue
of theFrobenius
Subgroup Theorem)
it is easy toanalyze Vm/2
when restricted toSpn
XSpn.
Indeed we know that the coset spaceSp2 n/Spn
XSpn
is anexample
of an affinesymmetric
space, and hence the orbit spaceP2nB Sp2n/Spn
XSpn
isfinite;
thus we can determine(Proposition 11.2.1)
afinite
Spn
XSpn composition
series forVm/2’
where the firstcomponent
of thecomposition
series is theSpn
XSpn
modulegiven by
the left andright
action on the spaceC~c(Spn).
Theimportance
of this observation is that"generically" Vm/2
as anSpn
XSp,
module has amultiplicity-one
property (Remarks
11.2.2 and11.2.3).
In 11.3 we use the
doubling principle
of the Weilrepresentation
toshow
(Proposition 11.3.1)
that there exists aninjective mapping
of thespace
(a
varies over allO(Qv) inequivalent, admissible,
irreduciblerepresenta- tions)
intoHomSpn Spn(03C1Qv, 03C0 03C0 03C0).
Thus we reducequestions
aboutmultiplicity
ofHomSpn(Kv) O(Qv)(S[Mmn(Kv)], 03C0 ~ 03C3) to studying
themultiplicity
ofHomSpn Spn(03C1Qv, 03C0 ~ 77).
However we notethat,
sincePQI’
does not in
general equal Vm/2,
we need finer information about theSP2,
module
Vm/2.
This wegive
inProposition
11.3.2.Finally
in11.4,
wegive
thestrategy
ofproof
of the local Howeduality conjecture
and the localmultiplicity-one conjecture
for the cases dis-cussed above. We introduce the notion of
Spn
XSp, boundary
compo- nents on the space03C1Qv
and prove thekey
technical step(Theorem 11.4.1)
that every
Spn
XSpn intertwining
operator from03C1Qv
to qr 0 qr which"lives" on a
boundary component will,
infact, imply
that qr or theassociated
03C0(03C3) (representation
ofO( Q ))
is eithernonunitary
or trivial.Then we must handle
computationally
the case where qr istrivial;
here we have toanalyze
aspecific Jacquet
module onS[Mmn(Kv)]
relative to aparabolic P,
inSpn .
§0.
Notation andpreliminaries
(I)
Let k be a local field of characteristic 0. We fix a nontrivial additive character T on k.Let,>k
be the usual Hilbertsymbol
on k. Let d x bea Haar measure on k which is self dual relative to T. We
let
be anabsolute value of k.
If k is
a, nonarchimedean field,
we let(2 k = ring
ofintegers
ofk,
03C0k = the maximal ideal in
(2k’ and q
= thecardinality
ofOk/03C0k.
(II)
Let K be a number field(i.e.
finitedegree
extension ofQ,
the rationalnumbers). Let AK
be thecorresponding
adelic group. Then embed K as a discretesubring in AK.
LetK v
be thecompletion
of Krelative to a
prime v
in K. Let r be a nontrivial character onAK
whichequals
1 onK ;
then there existcompatible characters rv
onKv (for
allprimes v
inK )
such that03C4(X) = 03A003C503C403C5(X03C5).
Let d X be the measure(Tamagawa measure)
onAK
such that the groupA KIK
is self dual relative to Tand A K/K
has mass 1. When the context isclear,
wedrop K in A K
andjust
use A for A K.(III) Let Q
be anondegenerate quadratic
form on K m. LetQv
be thecorresponding
local versions onKm03C5.
IfQ03C5
is atotally split
form which is the direct sum of rhyperbolic planes,
then we letQ03C5
=Hr.
LetO(Q)
bethe
orthogonal
group ofQ.
Then we can form thecorresponding
adelicgroup
O(Q)(A)
and thecorresponding
localorthogonal
groupsO(Ql’)
ofQv
atK,,.
LetO(Q)(K) = the
K rationalpoints
inO(Q)
and embedO(Q)(K)
intoO(Q)(A)
in the standard way. Choose aTamagawa
measure on the
quotient O(Q)(K)BO(Q)(A)
asgiven
in[Ar].
Similarly
let A be anondegenerate alternating
form onK 211.
LetSp,,
be the
corresponding symplectic
group andSpn(A), Spn(Kv)
the associ- ated adelic and localobjects.
LetSpn(K) =
the K rationalpoints
inSp,,
and embed
Spn ( K )
intoSpn(A) again
in the standard fashion and choosea
Tamagawa
measure on thequotient Spn(K)BSpn(A)
asgiven
in[Ar].
(IV)
We consider the category of smoothrepresentations
for the local andglobal objects
inquestion.
Thatis,
03C0v is smoothlocally
forG,, (a
localgroup)
if(1)
at the Archimedeanprimes,
77,, is a differentiable module forG,,, i.e., (03C0v)~
= COO vectors in ’lT1’=’TT1’ and(2)
at the finite non-Archi- medeanprimes,
03C0v is a smooth module forG,,
in the sense of[B-Z].
Thenwe consider also the
category
of admissible modules asgiven
in[B-Z]
and[B-J].
In the non-Archimedean case, we use the notion of
Jacquet
functorgiven
in[B-Z].
Thatis,
ifN,
cG"
is any closedsubgroup,
and if 03C0v is any smoothG,, module,
we have a functor from 17, to(03C0v)Nt
=03C0v/03C0v(Nv),
where
03C0v(Nv) = (all
linear combinations of the formx - 03C0v(n)x
as xvaries in 03C0v and n varies in
N,, 1.
Moreover we consider the category of admissibleGn
modules asgiven
in[F].
In this context, we note the well known relation in[F]
betweenunitary
irreducible modules ofGA
andadmissible irreducible modules of
GA.
We also use the notion of auto-morphic
irreduciblerepresentation
ofGA
asgiven
in[B-J].
(V)
LetX,,
bean espace
in the sense of[B-Z].
Then
S(Xv)
is the space oflocally
constant andcompact support
functions onXv.
IfX~
is a Coomanifold,
thenS(X~)
is the space of C’functions on
X~
which have anappropriate rapid
decreaseproperty (relative
toderivatives, etc.)
Then if X is the restricted directproduct 03A0v Xv,
thenS(X)
is the restricted tensorproduct 03A0vS(Xv)
in the sense of[F].
If S is any set of
places
ofK,
we letC°°(Xs)
be the space of smoothcomplex-valued
functions onXs,
andC~c(XS),
those elements inC~(XS) having compact support.
Note thatf
inC~c(XS)
is smooth iff
isf continuous on
Xs
and as a function of 2 variablesXS,~ iC Xs,fin
É C withf
in COO inX~ (locally
constant inXfin, resp.)
for fixed x~(xfin resp.).
For
instance,
we know that if X =Mmn(K), m
X n matrices overK,
thenScomp(XS1) ~ S(Xfin)
is dense inC~c(X),
whereSI
= set of Archimedeanprimes
ofK, Scomp(XS1) =
thecompactly supported
elements inS(XS1),
and fin = all finite
primes
in K.(VI)
IfGA
is aglobal
group, then we denote the space of cusp formson
GKBGA by L 2 cusp (GA).
We note(by
ourconvention)
that ifGKBGA
iscompact, then
L2cusp(GA) = f all
functionsf ~ constants}.
We know thatL2cusp(GA)
isdiscretely decomposable as a Gn module,
and eachunitary
irreducible
representation occurring
inL2cusp(GA)
has a finitemultiplicity.
We denote
where
dg
is someTamagawa
measure on thequotient G(K)BG(A).
(VII)
We consider thefollowing
Weilrepresentation. Namely
we fix anondegenerate form Q
on k m(k,
a localfield)
and anondegenerate alternating
form A onk2n. (Here
we havedropped
thesubscript v
fromQ
to avoid excessive
notation; throughout
the paper it will be clear from the context when thesymbol Q
is meant to denoteQv.)
Then we consider thealternating
formQ ~ A
onMm2n(k).
To this form we associate a Weilrepresentation
of the two-fold coverSPm.n
ofSpmn given
in[We].
Thenwe restrict the
representation
to asubgroup pn
XO( Q )
= inverseimage
of
Sp,
XO(Q)
inSPmn.
The
representation 77Q
ofSpn X O(Q)
isgiven by
where
y( )
isgiven
in[R-S-2]. Then,
if m is even, we know that there exists asplitting
mapSpn ~ pn(k), G (G, s2(G))
such that G(G, s2(G)) ~ 03C0Q(G, s2(G)) gives
arepresentation
ofSp, (see [R-1]
fordetails).
In the
case Q
=Q’ ~ (- Q’),
whereQ’
is anynondegenerate form,
it ispossible
to linearize the Weilrepresentation 77Q.
Thatis,
we define thepartial
Fourier transformHere we note that the action of
Spn(k)
isgiven by
where
03A9[X1] = [X1|X2]
and[XIX2]G" = [X’1|X’2]
withand
G = [A B].
C D Here we have theidentity
We note
that,
via achange
ofbasis,
that ifQ = 1 1,, /1 , then
thecorresponding
linearizationFT
isgiven by
(VIII) Using
the local data in(VII),
we can define aglobal
Weilrepresentation 03C0Q
ofSpn(A) O(Q)(A)
on the spaceS[Mmn(A)] (for details,
see[We]).
For every 99 ES[Mmn(A)],
we can construct a function((G, g) E SPn (A) X O(Q)(A»:
Then 0,
is anautomorphic
function onSpn(A) O(Q)(A).
Thatis,
03B8~(03B31G, 03B32g) = 03B8~(G, g )
for ally, E Spn(K), y2 E O(Q)(K). Moreover 0.
is a
slowly increasing
function onSpn(K)
XO(Q)(K)BSpn(A)
XO(Q)(A)
in the sense of
[B-J].
(IX)
We construct hererepresentatives
for the maximalparabolic subgroups
ofO(Q)
andSp,,.
(A) Sp,
hasparabolics given by Pn-1,
i =0,...,
n -1,
wherewith
and
and
Un1
is the semidirectproduct Un,1l Un,2l,
where
and
(B) O(Q)
hasparabolics given by Pr, r
=1,...,
indexQ,
wherewhere E ~ 03A3* ~
03A3r
= k m isa Q orthogonal splitting
of km into spaces where03A3, 03A3*
areQ isotropic subspaces
which arepaired nonsingularly by Q.
Here weidentify 03A3, 03A3*, and 03A3r
towhen we consider k m as a space of column vectors. Also
O(Q|03A3r) =
theorthogonal
groupof Q
restricted to thesubspace 03A3r, G~(03A3) =
thegeneral
linear group~ O(Q) operating
on E andby contragredience
onE*,
and
where the action on an element
(where
weview Q
as a formon 03A3r),
(X)
Given anautomorphic
formf
onSpn(A)
or ~ onO(Q)(A),
weknow that the constant term relative to a maximal
parabolic
isgiven by
on
Spn(A)
andon
O(Q)(A),
where du and du* are induced measures onU,"( K ) B U,"(A)
and
r(K)Br(A) having
normalized mass 1 for these compactquotient
spaces.
(XI)
The standard maximalcompact subgroups
ofSp,, G~m,
andO(Q)
are determined(up
toconjugacy)
as follows:(1) Spn(O03BB) ~ Spn(k), (ii) G~m(O03BB) ~ G~m(k),
(iii)
thesubgroup
ofO(Q) stabilizing
a lattice in km with a "Wittbasis", i.e.,
abasis {el}
of k "’ such that(a)
e1,...,er(er+1, ..., e2r, resp.)
generate over k maximalQ-iso- tropic subspaces
ofkm,
(b) Q(el, er+J) = 03B4tJ, 1 i r,
(c)
e2r+1, ..., em generate over k theQ-orthogonal
of the span{e1, ..., er, er+1, ..., e2r}
and generate theunique maximal (9, integral
lattice of this space.(XII)
Given anarbitrary, connected,
reductive group G, we let P’ be aminimal
parabolic subgroup
ofG,
and P, aparabolic
of Gcontaining
P’.Let A’ c P’ be a maximal
split
torus ofG, 4J
a rootsystem
of G with respect toA’,
and II a set ofsimple
roots of 4J. Then we say that theparabolic pair (P, A)
of G dominates(P’, A’)
if there exists a subset II’of II such that A =
largest
torus contained in the intersection of the kernels of the elements of II’. Forany 8
>0,
we letA-(03B4) = t a
EA~03B1a(a)| 03B4
for all roots a, in II -II’}.
LetP
be theopposed parabolic
to P in G.
We let N and
N
be theunipotent
radicals of P andP, respectively.
Let qr be an
admissible, finitely generated representation
of G. Letbe the
contragredient representation
of G. Weapply
theJacquet
functorsto qr and relative to N and
Ñ.
Then we know from
[C]
that(ir) Ñ
is thecontragredient representation
to 77,
(relative
to the connected reductivesubgroup
M of G whichsatisfies P = M - N and
P
= M ·N, semidirect).
Indeed we have the fol-lowing precise
version of thisduality. Namely
there exists aunique
M-invariant
nondegenerate pairing ·,· >N
between 77, and()
with thefollowing properties: given vi and v2
in qr and ,respectively, and 03C5’1
andU2
thecorresponding images
in 77, and(),
there is a realnumber Ej
> 0 such thatfor all a ~ A -
( e1 ).
1. Global
theory
91.
Constant termof 0-functions
We assume that m is even and
Q
anarbitrary nondegenerate form
on k "’.We fix cp E
S(Mmn(A»
and we consider the associated 0-seriesThen we know from
[20]
that as a function onSpn(K) O(Q)(K)B Spn(A) O(Q)(A), 03B8~
is aslowly increasing function,
i.e.for some
positive integer m, ~ ~ a
norm onSpn(A) O(Q) given
in[4].
The purpose of this section is to compute for any maximal
parabolic subgroup
ofSp,
orO( Q ),
the constant termof 0,,,
in the direction of thatparabolic subgroup.
First we consider thefollowing
maps:Then we construct the associated 0
functions, namely 0398l(03C0Q(G, g)W)
= 03A303BE~Mml(K)03C0Q(G, g)(~)[03BE|0] and
(see 90(VII)
and§0(IX)).
We than state the main Theorem which determines the constant terms.
We note that the
following
theorem is ageneralization
of the results of[R-2].
Inqualitative
terms, the contentpf
this Theorem isessentially
thatthe constant term of a lift
along
agiven
maximalparabolic
is the lift associated to a 0 series in a smaller number of variables.This,
infact,
isvery close to the use of the 03A6
operator
in thetheory
ofSiegel
modularforms.
THEOREM 1.1.1:
PROOF: We first note that
where
Wl = {X ~ Mmn(K)|X’QX = [* 0], * arbitrary
i imatrix}
(see§11.4).
Then we consider the orbits of
O(Q)(K) Zl(K) in Wl,
whereZl(K) = {(A 0)|A ~ G~l(K), B ~ G~n-l (K),
and *arbitrary}
c
G~n(K).
The set oféquivalence
classes of such orbits isparametrized by
thefollowing
set ofrepresentatives:
where
e,, .... 03BEt
form a nonzero,linearly independent
set ofmutually Q isotropic
vectorsspanning
thesubspace E (see §0 (IX) (B)),
and X runsthrough
a set ofrepresentatives
ofO(Q|03A3t) G~l
orbits inMm-21,(K) (with m -
2 t =dim 03A3t).
We note that the number of suchO(Q)(K)
XZ, ( K )
orbits inW
is finite.Then we have that
where
Zl(K)[X|03BE]
= stabilizer of[X|03BE]
inZl(K)
andPt
= the maximalparabolic
inO(Q)(K) given by O(Ql03A3t)(K) G~m-2t(K) t(K)
(which
inO(Q)(K)
is the stabilizer of theZ, ( K )
orbit of[X|03BE]).
Thus wehave that
Here
But then we note that
Zl(K)[X|03BE] splits
as a semidirectproduct
of 2groups:
and
Thus we have that
Hence we have
by (formally) integrating 03B8(Pn-1)~ against
a cuspform f
on
O(Q)(K)BO(Q)(A),
where
LtK
=O(Q|03A3t)(K)
XG~m-2t(K).
But we note that the functionis
Nt(A)
invariant ! Thus the innerintegral
above ismerely f(Pt)(g)
= theconstant term
of f in
the direction of theparabolic t
inO( Q ). But f is cuspidal implies
that the above sum vanishesif e
is not the zero matrix !Thus we have that
for all G.
Although
theproof
of(2)
is very similar to that of(1),
we include theproof
toemphasize
theimportance
of thelinearizing property
of the Weilrepresentation (see §0(VII)).
Inparticular
we have thatwhere
FTr
is thepartial
Fourier transform "relative to03A3r" given by
for (p E
S[Mmn(A)] (see §0(VII))
and(see §0(IX)).
But
then,
similar to(1) above,
we note that theG~r(K) Spn(K) orbits in {[R|S]|RSt symmetric with R, S ~ Mrn(K)} = {X ~ Mr2n(K)|X
0 In] Xt = 0}
aregiven by représentatives
of the formVl = [Il|0]
with i =
0,..., min( n, r ) (with I,
= 1 X iidentity matrix).
Thus we have
(formally)
thatwhere
G~r(K)Vl
= Stabilizer of theSpr(K)
orbitof V,
inGtr(K).
Herewe have used the fact that
03B31r(T) = r(T03B31)03B31
andd(Ty) =
Idet 03B3|Kd(T)
=d(T)
onMm-2r,r(K)BMm-2r,r(A).
Then we have
(using
the definition ofNr
in§0(IX))
But then the latter
integral
vanishes if andonly
if X ·I,’
= 0. Thatis,
X ·
Il
=[Xl|0]
= 0 if andonly
ifX,
= 0.Then we note that
as a function of G is invariant on the left
by
thesubgroup
ofStabA(Vl) isomorphic
toBut this latter group is the
unipotent
radical of a fixedparabolic subgroup
ofSPn (K).
Then we canapply
the samereasoning
as in(1)
anddeduce (2). Q.E.D.
Appendix to §1
We must prove the absolute convergence of the
following:
This allows us to switch orders of
integration
when we compute in 1.1 theintegral
But we note that
O(Q)(A)
=P(A) . K,
where K is a compactsubgroup
ofO(Q)(A).
Then( A )
ismajorized by
a finite number of terms of the formwhere (p,
and(î, belong
toS[M2t,n(A)]
andS[Mm-2t,n(A)],
resp.and f,
isa cusp form on
O(Q)(A).
Note
17,,
and77Q are
the Weilrepresentations
of thepairs O(QI)
XSp,,
on
S[M2t,n(A)] (where Q1
= the restriction ofQ
to 03A3~ 03A3*, i.e.,
see§0(IX)(B))
and(O(Q|03A3t)
=O(Q2))
XSPn
onS[Mm-2t,n(A)].
But then weuse the
rapid decreasing properties
off,
to deduce the absolute conver- gence of the above series!§2.
Howeduality conjecture
Thus as a consequence of Theorem 1.1.1 we deduce the
following corollary.
COROLLARY TO THEOREM 1.1.1:
(a)
Letf E L2cusp(O(Q)(A)). Then 03B8~(G, 9)|f(g)>O(Q)(A)
is a cuspform
onSPn(K)BSPn(A) if
andonly if
( e 1 ( ’TT Q ( G, g)(~))|f(g)>O(Q)(A) ~ 0
for
all G ESpn(A)
and i =1,...,
n.(b)
Letf * ~ L2cusp(Spn(A)).
Then(0,(G, g)|f*(G)>Spn(A)
is a cuspform
onO(Q)(K)BO(Q)(A) if
andonly if
l(03C0Q(G, g)(~))|f*(G)>Spn(A) ~
0for
all g~ O(Q)(A)
and i =1,..., index(Q).
REMARK 1.2.1: We note here that a
simple
exercise willverify
that0398l(03C0Q(G, g)(~))|f(g)>O(Q)(A)
~ 0 for all G ESpn(A)
and all ~ ES[Mmn(A)]
isequivalent
to03B8~(G, g)|f(g)>O(Q)(A) ~
0for all G E
Spl(A)
and all cr ES[Mml(A)].
A similar statement holds forl(03C0Q(G, g)«p» given
above.Then we define the
subspaces Lr(Q) = {f ~ L2cusp(O(Q)(A))
2|03B8~(G, g)|f(g)>O(Q)(A) ~
0 for all G ESp,(A)
andall ~ ~ S[Mmr(A)]}
(recall
here that0,
is the 0-function associated to the Weilrepresentation
of
SPr
XO(Q )
onS[Mmr(A)])
andI(Q) = ( f*
eL2cusp(Spn(A))|03B8~(G, g)|f*(G)Spn(A) =
0 for all g ~O(Q)(A)
and allcr E
S[Mmn(k)]},
m = dimQ.
Then we define
inductively R1(Q) = L1(Q)~
inL2cusp(O(Q)(A)),
R2(Q) = (LI (Q)
nL2(Q»-L
inL1(Q),..., Rl(Q) = (L1(Q)
n... Ll(Q))~
in
L,(Q)
nL2(Q)
n...Ll-1(Q). Similarly
letI1(Q) = I(Q)~
inL2cusp(Spn(A)), I2(Q) = (I(Q)
nI(Q ~ H,» 1
inI(Q),... , Il+1(Q) =
(I(Q)
nI(Q
~Hl)... ~ I(Q ~ Hl))~
inI(Q) ~ I(Q ~ H1) ~ ... I(Q
~Ht-1).
Here weadopt
the convention that ifQ
is the zeroform,
thenII(Q) = foi.
Then we have the
following
Structure Theorem about the cusp formson
Spn
orO(Q).
THEOREM 1.2.1:
(1) L2cusp(O(Q)(A)) is an orthogonal
direct sumof R1(Q) ~ R2(Q) ~ ... ~ Rm(Q)
where m = dim
Q.
(2) Let Q be an anisotropic form
over K. ThenL2cusp(Spn(A)) is
anorthogonal
direct sumof
I1(Q) ~ I2(Q ~ H1) ~ ... ~ Ir+1(Q ~ Hr)
where r = 2 n .
PROOF:
(1) By employing Corollary
to Theorem 1.1.1 and Remark1.2.1,
we have that
L2cusp = R1(Q) ~ ... Rl(Q) ~ L1(Q) ~ L2(Q) ~
... ~ Ll(Q).
Then it suffices to show thatL1(Q) ~ ... ~ Lm(Q) = (0).
Indeed we show that
Lm(Q) = (0).
First we note thatO( Q)(A)
embeds asa closed subset of
Mmn(A) (for n? m )
viaO(Q)(A)
~ {(B 0)|B ~ O(Q)(A)} ~ Mmn(A).
Moreover the restriction mapC~c(Mmn(A)) ~ C~c(O(Q)(A))
issurjective.
Then we note that every function inC~c(O(Q)(K)BNO(Q)(A))
is obtainedby averaging
a functionin
C~c(O(Q)(A)), i.e., H ~ C~c(O(Q)(K)BO(Q)(A))
has thé form03A303B3~O(Q)(K)~(03B3 · x), x ~ O(Q)(A)
and ~ EC~c(O(Q)(A)).
Thus, if f in L2cusp(O(Q)(A))
has theproperty that f|H>O(Q)(A) ~ 0.
for a dense set of H
above,
thenf ~
0.Then
if ~
ES[Mmn(A)],
we deduceeasily
thatwhere
~Q= [Q 0].
But we note that{03BE ~ Mmn(K)|03BEtQ03BE = ~Q} =
But we know that
S[Mmn(A)]
containsScomp(Mmn(K~)) ~ S[Mmn(A fin)] (see §0(V)),
which is dense inC~c(Mmn(A)),
and theimage
of
S [ M,,,,, (K.)] 0 S[Mmn(A (via restriction)
inÇ’ (O(Q)(A»
is densein
C~c(O(Q)(A)).
Henceif f ~ Lm(Q),
thenf|03B8Pn,~Q~(G, )>O(Q)(A) ~ 0
for all cp E
S[Mmn(A)];
thisimplies by
the comments above thatf ~ 0.
(2)
Weapply
a similarargument
as above. First we note thatSpn(A)
embeds as a closed subset of
M03BBn(A) (with 03BB 203BC 4n, where tt
= Wittindex of
Q)
viaSpn(A) ~ {[03A9-1G03A9(Xn) 0]} |G ~ Spn(A) } ~ M03BBn(A), with In
Xn = 2.- (see 11.1).
Thenif ~ ~ S[M03BBn(A)],
we deduce that the Fourier0
In
coefficient
of 0,
in the direction of the centralsubgroup Z03BC(s) =
{03BC((0, s))|s
a Il X jn skewsymmetric matrix}
of theunipotent
radicalfi,
in
O(Q)(A)
relative to the skewsymmetric
matrix0 In
A = [- In 0 0
0
0
is
given by
where
03C0l( )
operateslinearly
onS[M2rn(A)] (see §0(VII)).
Thus
following
the samereasoning
as in case(1),
we deduce that iff* ~ I(Q
E9Hr-1) (where r 2n ), then f*|03B8Z03BC,A~(G, g)>Spn(A)
= 0 for allcp E
S[M03BBn(A)]; thus f*
= 0.Q.E.D.
REMARK 1.2.2: We have shown that in
(1) Lt(Q)
={0}
if t à m and in(2) I(Q
E977,)= {0}
if r 2n.Then for a fixed
cuspidal representation
03C0occurring
inL2cusp(O(Q)(A)),
we consider the
subspace
Here
(qT)
denotes theisotypic
component inL2cusp(O(Q)(A))
whichtransforms