C OMPOSITIO M ATHEMATICA
S TEPHEN S. K UDLA
On certain Euler products for SU(2, 1)
Compositio Mathematica, tome 42, n
o3 (1980), p. 321-344
<http://www.numdam.org/item?id=CM_1980__42_3_321_0>
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321
ON CERTAIN EULER PRODUCTS FOR
SU(2, 1)
Stephen
S. Kudla*COMPOSITIO MATHEMATICA, Vol. 42, Fasc. 3, 1981, pag. 321-344
(c) 1981 Sijthoff & Noordhoff International Publishers - Alphen aan den Rijn Printed in the Netherlands
Introduction
In a recent paper
[12]
Shintaniinvestigated
the Eulerproducts
associated with
automorphic
forms onSU(2, 1)
which areeigen-
functions on the Hecke operators. He
showed,
inparticular,
how theaction on the Hecke operators transforms the Fourier-Jacobi series of such forms and gave an
integral representation
of the associatedDirichlet series with Euler
product.
Such anintegral representation
with Euler
product
was also consideredby Piatetski-Shapiro [7].
On the otherhand,
there is alifting
fromordinary elliptic
modular forms toautomorphic
forms onSU(2, 1),
definedby
a certain theta function of two variables[4].
In this paper we show that the lift of a Heckeeigenform
isagain
a Heckeeigenform
and that the Dirichlet series of the lift has a niceexpression
in terms of that of theoriginal
form. Ineffect we show that the
lifting
inquestion
iscompatible
withLang-
lands’
principal
offunctoriality.
More
precisely,
let K =Q(i),
let o, be the Galoisautomorphism
ofK/Q,
and letThen
2 iR
defines a Hermitian form ofsignature (1, 2)
on V =K3.
Let* Partially supported by NSF Grant MCS78-02817.
0010-437X/81/03321-24$00.20/0
be the group of similitudes of
R,
and letbe the
corresponding
Hermitiansymmetric
space.Let O = Z[i],
andfor the lattice L = O3 C
V,
letFor g
EG(R) and 03B4
ED,
setwhere
(a3, b3, c3)
is the bottom row of g. Then forany k
EZ, k
> 5 and k =0(4)
there is alifting
where
Sk-,(Fo(4), (-4))
is the space of cusp forms ofweight k -
1 onSj,
the upper halfplane,
andAk(G(L))
is the space ofholomorphic
functions F on D
satisfying
for
all g
EG(L).
Our
result
is thefollowing:
Iff(03C4) = 03A3~n=1 a(n)e(n03C4) ~ Sk-1(.ro(4), (-4))
is a Heckeeigenform,
then so is2(f),
andwhere
03B6(s, ~, F)
is the Dirichlet séries attached to a form onD, L(s, f) = 03A3~n=1 a(n)n-S, f03C1(03C4) = 03A3~n=
1a(n)e(n03C4), and X
is the grossen- character of K definedby
Now the function
03B6(s,
X,F)
is the L-function of Fassociated, by Langlands [5],
to a certainrepresentation
p of theL-group
of G. If welet
323
where
then there is a
homomorphism a : LH~LG
ofL-groups
suchthat, locally,
with theexception
of the Euler factorfor p
=2, C, (s,
X,0( f))
is the Euler factor associated to
f
for therepresentation
p - a ofLH.
Our
proof
of(0.1)
is based on the classicaltechnique
usedby
Eichler[2,
Satz21.3]
to relate the actions of Heckeoperators
andgeneralized
Brandt matrices in spaces of 0-functions. On the otherhand,
Rallis[8]
gave arepresentation
theoreticproof
of Eichler’s result. In[9]
Rallisapplied
his method to check localfunctoriality
forthe
correspondences
determinedby
the Weilrepresentation
for thedual reductive
pair (Om, Spn).
It should bepossible
to extend Rallis’method to the dual reductive
pairs ( U( V), U( V’)).
The existence of a
holomorphic analytic
continuation and func- tionalequation
fore(s,
X,:£(f))
is an immediate consequence of(0.1). Eventually
theseproperties
will be obtainable for all Fby
themethod of Shintani and
Piatetski-Shapiro.
In § 1 we
specialize
themachinery
of[4]
to the present case. We then recall the definition of the Heckeoperators acting
inAk(G(L))
and state the
theorem,
which relates the action of the Hecke opera-tors on the two variables of the theta function
defining
thelifting.
This theorem has the above relation between Dirichlet series as an
immediate consequence. The
proof
of the theorem isgiven
in §2. In§3,
we discussfunctoriality.
1 would like to thank Professor Shintani for a conversation which stimulated this paper, and Professor M. Karel for his advice about
LG.
§1.
Thelif ting
and Heckeoperators
Let
K, R, G, D,
etc. be as in theintroduction,
and define a Her- mitian form on Vby
Note that this is the
negative
of Shintani’s form. For L C V asbefore,
let
be the dual lattice. Here
tr(03B1)
=trK/Q(03B1), 03B1
E K.Also, for 03B4
ED,
letand let
and let
Now
for 03B4
ED,
the vectorP (3)
E V spans apositive
line inV;
and wemay define the
majorant (,),
of(,)
associatedto 03B4 by
Then
for k ~ Z > 0, h
E L* and03C4 = x + iy ~ L,
setAccording
toProposition
2.1 of[4],
if y= (a d) ~ Fo(4)
thenwhere
03C8(d) = (sgnd)(-4 |d|)
is thequadratic
character associated toK/Q.
Alsoif g
eG(L),
Set
8(T, 3)
=8( T, h, 0)
and suppose that k = 0 mod 4 so that8(T, 03B4)
~ 0.Then
by
Theorem 5.3 of[4],
iff
ESk-1(03930(4), 03C8)
and k > 5 the func- tion325
is a
holomorphic
form on D ofweight k
withrespect
toG(L);
L(f)
EAk( G(L»).
Note that the
automorphy
factorJ(g,03B4)k corresponds
to the case1
= k, m
=0,
d = 0 in Shintani p. 2[12].
Now we recall the definition of the Hecke
operators
for G follow-ing
Shintani[12].
For aprime
P of K with P =(?r),
1T EK,
define a subsetS(P)
CG(Q)
as follows:(1) If P ~ P03C3, p = PP03C3, let
S(P)
=f g
EM3(O)
~G(Q) |03BC(g)
= pand g
haselementary
divisors(2)
If P = pu, letThen
S(P)
is a union ofG(L)
double cosets and may be written as afinite
disjoint
unionFor F E
Ak(G(L))
defineThe
T(P)’s
generate a commutativealgebra
of operators onAk(G(L)).
If F EAk(G(L))
is a simultaneouseigenfunction
of all theT(P)’s
withand
if e
is agrossencharacter
ofK,
then there is a Dirichlet series with Eulerproduct
associated to Fand e
in thefollowing
way:and
where X =
~(P) = ()k.
Define the Euler factor at pa
(2)
If P = pu =(p )
is unramified inK/Q,
setand define the Euler factor at p
where E =
(-I)k/4,
and setThen define
Also recall that if
f
ESk-,(FO(4), 03C8),
the Heckeoperator T’(p)k-1,03C8
acts
on f via
where
03C8(2)
= 0. In the notation of[ 11; (3.4.1)],
setwhere 0393’ =
Fo(4).
Now our main
result,
to beproved
in the nextsection,
describes theaction the
T(P)’s
on the theta function03B8(03C4, 03B4).
THEOREM:
(1) If
P ~P03C3,
P =(7r),
then[7]
(2) If
P = P" isunramified in K/Q.
Then(3) If P = (1 + i),
thenREMARK: The theorem is an
analogue
of a classical result of Eichler[2,
Satz21.3]
and the method ofproof
is similar to his. The thoerem is anexplicit special
case of thegeneral
results of Howe[3].
COROLLARY 1:
Suppose
thatf
ESk-l(ro(4), 03C8)
is a normalizedHecke
eigenform
such thatL(f)
~ 0. ThenL(f)
is aneigenfunction of
all the
T(P)’s
witheigenvalues given by :
where X =
~(P) = ’r
in thefirst
case, and E =(_1)k/4.
PROOF: This follows
immediately
from the theorem and well knownadjointness properties
of the Hecke operators withrespect
to the Petersson innerproduct (,). Note
thatL(f)
=( f, 0)
and that(1
+i)k
=~2k/2.
COROLLARY 2: For a normalized Hecke
eigenform f
ESk-l(ro(4), «/1)
such that
L(f) ~ 0,
we havewhere
LK(s, X)
is the Hecke L-seriesfor
thegrossencharacter
X andL(s, f )
is as in the introduction. Thus thefunction
has an entire
analytic
continuation andsatisfies
thefunctional
equa- tion :where
G2(S) = (203C0)1-sT(s).
PROOF: If P ~
pu,
we substitute the valuesgiven
in Cor. 1 for 03BB(P) and A(P’)
intoQ1(X)
and obtainSimilarly
forQ2(Y)
we getNow
setting
X =Xp k/2-s
and Y =Xp k/2-s yields
and
Since
à,
=.p(p )ap
= ap, we get, after a shift ofk/2
in s, therequired identity
on Euler factors.Similarly
if P = P03C3 =(p)
isunramified,
the value for03BB(P) given
inCor. 1
yields
for
Q(X);
andputting
X =pk-2s gives
Since
ap=03C8(p)ap=-ap
this is therequired identity, again
with ashift of
k/2
in s.Finally,
if P =(1
+i )
we obtain329
Setting
X =~((1
+i))2k/2-s
andnoting
that~((1
+i»
= E, we getwhich is
just
since a2à2 =
2k-2, [6].
The functional
equation
ofD(s, X, 5t(f))
followsimmediately
fromthose of its factors.
§2.
Proof of the TheoremFor g
EG(Q),
let g =1£(g)g-’.
Then g ~G(Q), (gX, Y) = (X, g’Y)
and
03BC(g’) = g(g). Also, G(L)’ = G(L) and;
since L is a maximal lattice in the sense of[10],
the setf g
EG(Q) |gL
CL}
is also stable under t.Now let
S(P) = ~j G(L)g;
asbefore,
and for X E L setNote that the
gjL’s
are certain sublattices of Lindependent
of thechoice of coset
representatives;
and that themultiplicities m(P, X) only depend
on theG(L)
orbit ofX,
sinceG(L) simply permutes
the sublattices inquestion.
For convenience write
Then
applying T(P)
toO( T, h) yields:
where we use the
identity
and the fact that
03BC(g)
=N(P)
forall g
ES(P).
Next we must
compute
themultiplicities m(P, X).
For each rational
prime
p, letKp
=K Q9Q Qp, Op
=O~Z Zp, Vp
=Kp
and
Lp
=t’.
Also letGp
=G(Qp)
and letThen for a
prime
P of Kwith p
= P nQ,
setso that
S(P)p
CGp, G(L)pS(P)pG(L)p
=S(P)p,
and in fact the above union is stilldisjoint. For p’ ~
p,so that
and
where now the
g;’s
can be any set of cosetrepresentatives
forG(L)p
in
S’(P)p.
Further observe that ifordp 03BC(gj)
= a, thensince
and
03BC(gj)-1p03B1
is a unit of6p. By
the same argumentm(P, X) only depends
on X modpa Lp.
PROPOSITION:
(1) Suppose
that P ~ pu, P =(ir).
Let331
Then
(2) Suppose
that P = pu =(p)
isunramified.
Letand
Then
(3) Suppose
that P = pu isramified,
so P =(03C0),
17" =(1
+i),
andp = 2. Let
and
Then
PROOF:
By
the aboveremarks,
the functionm(P, X)
isactually
defined on
Lp/ N(P)Lp
and is constant onG(L)p
orbits in this set.Therefore to compute
m(P, X)
we needonly
find a set ofG(L) p
orbitrepresentatives
and a set of cosetrepresentatives
gj.(1)
If P ~P03C3,
P =(1T)
with 1T EKp,
and takeidempotents e
and e’in
Kp.
Thenand
Note that we may assume that 7r is chosen so that the
corresponding
element of
Qp
xQp
is[p, 1].
SetRI
= eR,R2
= e03C3R. Thensince
g2 = cg*
withgt
=R-’gIR2, gl
=tg-11.
The action of[g, c]
EGL3(Qp)
XQp
on[X, Y]
EQp
xQp
isgiven by
Since
R2
EGL3(Zp),
The above action is
equivalent
to the "standard" actionunder the
isomorphism 1 R2:Q3p Q3p~Q3p Q3p.
It is then easy todetermine orbit
representatives
forGL3(Fp) Fxp,
and hence for333
G(L),,
inFor
example,
we may takeand these
correspond
to the casesCl, Co+, Co-, Coo,
and ’otherwise’above.
Now Shintani
[12,
Lemma2],
found a nice set of coset represen- tatives forS(P’),IG(L),.
For w EKp
and u EQp,
setand let
Then
H(L) p
CG(L) p,
and Shintaniproved
thatIt follows
easily
thatgive
a set of cosetrepresentatives
forS(P03C3)p/G(L)p
where w runsover
representatives
forOp/7TOp
and u runs overrepresentatives
forZp/pZp.
SinceS(P03C3)p
=S’(P)p,
we may take the aboverepresentatives
as our
g;’s.
Theimages
of theseg;’s
inGL3(Q p )
xGL3(Qp)
under theisomorphism corresponding
to the above "standard" action will beand
where a and b run over a set of
representatives
forZp/pZp
and theimage
of 2i inQp
xQp
is[03C9, -03C9)].
The
images
of these elements inM3(Fp)
xM3(Fp)
have cokernels of dimension3,
and themultiplicities m(P,X) given
in(1)
of the pro-position
are obtainedby counting
the number of these cokernels which contain X. We may, of course, take X to be one of our orbitrepresentatives
above.If P = P03C3 =
(p)
isunramified,
we must determineG(L) p
orbits inLp/p2Lp.
First observe that there areprecisely
threeG(L)p
orbits inLp/pLp represented by 0, ’(0,1,0),
andt(0, 0, 1).
In factand R determines a
non-degenerate
Hermitian form on this space. IfG,
is the group of similitudes of thisform,
thenand so
Gp,
and henceG(L) p,
actstransitively
on{X ~
LP/pLp |(X, X) ~
0 modp}.
If X EF)2
with(X, X)
= 0 but X ~0,
thenwe may
complete
X to a Witt basisX, Y,
Z forF)2
with(X, Y)
=1,
( Y, Y) = (X, Z) = ( Y, Z)
= 0 and(Z, Z)
= 1. Thus such X form asingle G(L)p
orbit.Now suppose that
X E Lp/p 2Lp
with(X, X) ~ 0 mod p2
butXÉ
pLp.
Then there exists g EG(L)p
such thatand a = 1 + px3 E
Cx.
Then335
where
The condition
( Y, Y)
= 0mod p2
isequivalent
toand hence
Therefore
with b E
Zp,
and soThis shows that the set
CI
in(2)
of theproposition corresponds
to asingle G(L) p
orbit inLp/p2 Lp;
andby
theprevious remarks,
the setbreaks up into three orbits
corresponding
toCo, Coo
andCooo
above.(2)
LetH(L) p
be as before. Then Shintani shows thatwhere c runs over a set of
representatives
forZ,lp7,p.
It followseasily
thatare a set of coset
representatives
forS(P),IG(L),,
where a runs overZp/p2Zp,
b runs overûplpcp,
and c is as before. SinceS(P))p
=S(P)p
in this case, we may take these coset
representatives
as theg;’s.
Again
if we consider the cokernels of theseg;’s acting
inLp/ p2 Lp,
wefind the claimed values for
m (P, X)
as the number of such cokernels which contain X.(3) Finally
in the case P = P03C3 isramified,
so P =(03C0),
1T= (1
+i),
p =
2;
there are in fact 11G(L)p
orbits inLp/pLp
for which we maychoose
representatives t(1
+ ir,0, 0), t(1
+ 7r,03C0, 0), t(1, 1T,0),
andt(1, 0, 0) corresponding
toC1; t(1T, 0, 0) corresponding
toCo; t(O, 1T,0) corresponding
toCoo;
0corresponding
toCooo,
andt (1, 0, 1T), t(03C0, 1, 0), t(0,1
+1T,0)
andt(0, 1, 0) corresponding
to ’otherwise’.Applying
Lemma 2 of
Shintani,
we find cosetrepresentatives
and
for
S(P)p/G(L)p. Using
these as ourgj’s - again S(P)tp
=S(P)p -
we cancompute the
m (P, X)’s
as in theprevious
cases, and theproposition
isproved.
REMARK:
Although
we have consideredonly
the case K =Q(i),
theproof
of theprevious proposition,
at least in cases(1)
and(2),
isidentical for an
arbitrary quadratic
extensionK/k.
Therefore both the337
theorem of § 1 and the
resulting
relation between the L-series of the lift and that of theoriginal
form should hold in thegeneral
case.PROOF OF THE THEOREM: We use the values for
m(P, X) just
determined.If P ~ pu, P =
(03C0)
with 77-E K, (2.2)
becomesOn the other
hand,
Since
the first term on the
right
side of(2.3)
isjust p2
times the first term onthe
right
side of(2.4).
Also we haveso that this term is
just p2
times the last term in(2.4).
NowSo that
and the first part of the theorem is
proved.
If P = P’ =
(p)
isunramified, (2.2)
becomes:while
If we write
AI, A2,
A3 and A4 for the four terms on theright
side of(2.5)
and
Bi,
B2 and B3 for the terms on theright
side of(2.6); then,
as in theprevious case;
At the same time
so that
Finally
and so
as claimed.
339
If P =
(1
+i),
p =2; (2.2)
becomes:while
Thus the first term on the
right
side of(2.7)
isp203B8|1 T’(p)k-l,.
Thesecond term on the
right
side of(2.7)
isFinally,
we note that if 0393’ =r,(4),
so that
Since for h E
L*,
and
we obtain
where
Then the second term on the
right
side of(2.9)
isjust
On the other
hand,
in the last term on theright
side of(2.7)
we have:Finally, setting
ir = 1 + i andwriting
X =03C0 Y,
we have:Setting Y’ = p-103C0Y
we have:hence
and
(2.10)
becomesThis
completes
theproof
of the theorem.§3.
Functoriality
Let G and H be the reductive groups over
Q
defined in the introduction.Following
the notation of[1]
we find thatand that the action of 03C3 is
given by
341
where g
=tg-1
andThen we take LG =
LG0 03C3>. Similarly
and the action of a is
given by:
Let LH =
LH0 03C3>.
Now the Euler
product
consideredby
Shintani arises in the follow-ing
way. LetpO by
the 3-dimensionalrepresentation
ofLaO given by
and let
Let
If F E
Ak(G(L))
is a Heckeeigenform
witheigenvalues À(P)
andcentral
character X
asin § 1, representatives in LT0 03C3p
of the cor-responding semi-simple LG0-conjugacy
classes inLG’
x (Tp are deter- mined as follows.If p
=PP03C3,
with P ~ pu inKI Q,
and
and
Note
that,
in the latter case, the condition that t be (T-invariant forcest2
= 1 andt-13
= t1 as well.We then find
that,
forp ~ 2,
Shintani’s Euler factor iswhere (Tp is the Frobenius in
Gal(K/Q)
at p.We now construct an
L-homomorphism.
First define03B10:LH0 ~ LG0 by
for h =
c d
ab
EGL2(C).
This can be extended to ahomomorphism 03B1: LH~LG by taking
Finally,
to a normalized Heckeeigenform f
ESk-1(03930(4), Ç)
weassociate,
for eachp, p ~ 2,
thesemi-simple LH°-conjugacy
class inLH0
Oprepresented by
the elementwhere
and Op is the Frobenius at p. Here
343
and
We then find
that,
forp ~ 2,
theeigenvalue 03BB(P)
associated to03B1(s 03C3p)
E ’T’X1lTp
isjust
as inCorollary 1,
and thatThis shows
that,
in the notation of[l, 7.2],
for classical Hecke
eigenforms f
ESk-1(03930(4), Ç),
and hencethat,
for such forms the Weilrepresentation
defines aglobal lifting compatible locally
at almost all p with theL-homomorphism
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New York, 1974.
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52 (1979), 1-25.
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[8] S. RALLIS: The Eichler commutation relation and the continuous spectrum of the Weil representation, Proc. of Conference on Non-commutative Harmonic Analy- sis. Lecture Notes in Math. 728, Springer, New York, 1979, 211-244.
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(Oblatum 18-VII-1979 & 30-V-1980) Department of Mathematics and
Institute for Physical Sciences
and Technology University of Maryland College Park, Maryland
20742