C OMPOSITIO M ATHEMATICA
J OACHIM S CHWERMER
On arithmetic quotients of the Siegel upper half space of degree two
Compositio Mathematica, tome 58, n
o2 (1986), p. 233-258
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233
ON ARITHMETIC
QUOTIENTS
OFTHE SIEGEL UPPER HALF SPACE OF DEGREE TWO
Joachim Schwermer
@ Martinus Nijhoff Publishers, Dordrecht - Printed in the Netherlands
§0.
IntroductionIn the arithmetic
theory
ofautomorphic
forms withrespect
to con- gruencesubgroups
r of thespecial
linear groupSL2(k)
over analge-
braic number field the
study
of variouscohomology
groups attached to r is very useful. Thisapproach
combinesanalytic,
arithmetic andalge- braic-geometric
methods and hasled,
forexample,
to the results ofLanglands [14]
or to those of Harder[8], [9], [10]
on arithmeticproperties
of
special
values of L-functions attached toalgebraic
Hecke characters.As one
aspect
of thisstudy
oneanalyzes
the de Rhamcohomology
groups of the associated arithmetic
quotient 0393BX (where X
denotes thecorresponding symmetric space)
and their relation toautomorphic
forms.Here the connection with the
theory
of Eisenstein series asdeveloped by Selberg
andLanglands [15]
is ofparticular
interest. First ofall,
thistheory
allows us to constructcohomology
classes which arerepresented by
values of Eisenstein series and whichcompletely
describe thecohomology of fBX
atinfinity, i.e.
thatpart
ofthe. cohomology
of theBorel-Serre
compactification 0393BX of 0393BX
which restrictsnon-trivially
to the
cohomology
of itsboundary ~(0393BX). Moreover,
these Eisensteincohomology
classes haveinteresting algebraic
or arithmeticproperties
which
led,
forexample,
to the results mentioned above.One may ask if and how these ideas can be
generalized
to othergroups. There are some results in
particular
cases(cf. [7], [10], [21], [22], [23])
but for groups of Q-rankgreater
than one there is nocomplete understanding
of the Eisensteincohomology.
Inparticular,
those groupsare of interest for which the de Rham
cohomology
of r has aninterpretation
in étaletheory
i.e. ascohomology
of anunderlying
arith-metic
variety.
The
object
of this paper is tobegin
thestudy
of these ideas in the caseof an arithmetic torsion free
subgroup
r cG(Z),
G =Sp4
thesymplectic
group of
degree
two. The associatedsymmetric space X
is theSiegel
upper half space of
degree
two, and thecorresponding
arithmetic quo- tient0393BX
is a 6-dimensionalnon-compact complete
Riemannian mani-fold of finite volume.
By
thegeneral
construction of Borel andSerre [3]
it can be viewed as the
interior
of acompact
manifold0393BX
withcorners. Its
boundary ~(0393BX)
is adisjoint
union of facese’(P)
corre-sponding
to ther-conjugacy
classes of properparabolic Q-subgroups
ofG. The
G(Q)-conjugacy
classes of theseparabolics
fall into threeclasses,
two
conjugacy
classes.91
andY2
of maximalparabolic subgroups
andone class
.90
of minimal ones. Then the first result is thatwhere Y
is theunion of
thee’(P)
withP ~Ji (modulo F)
and itscompactifications Y,, Y2
are 5-dimensional manifolds with commonboundary Yo.
By
ananalysis
of theMayer-Vietoris
sequence associated to thedecomposition (1)
we determine in 2.7 thecohomology
of theboundary
8(rNX).
Moreprecisely,
ifr = r( m ), m 3,
is a fullcongruence subgroup
ofSP4(Z)
wegive
adescription
ofH*(~(0393BX), C)
as arepresentation
space for the finite groupfG = Sp4(Z)/0393(m).
It consistsof induced
representations
fromsubspaces
of thecohomology
of theindividual faces in
~(0393BX) (which
is described in2.5.) together
withsome
"non-geometric" pieces.
Out of this result we derive a formula(2.9)
for the dimension of theimage
of the restrictionof the
cohomology
of0393BX
onto thecohomology
of itsboundary.
Theformula involves
only
the dimensions of the spaces of cusp forms ofweight
k =2, 3,
4 withrespect
to the congruencesubgroup
of level m inSL2(Z)
and the number ofr( m )-conjugacy
classes ofparabolic
Q-sub-groups P in
Ji,
i =0, 1, 2,
all of which can beexplicitly computed
interms of m. We are very brief in the
proofs
of§2
since theinvestigation just
described runsmethodologically along
similar lines as forSL3/Q
(cf. [16], [22] §7) though
there are some new features.As
indicated,
thetheory
of Eisenstein seriescan
now beused
toconstruct
by analytical
means asubspace H*Eis(0393BX, C) in H*(fBX, C)
which is
generated by
Eisensteincohomology
classes(i.e.
classes with arepresentative given by
aregular
value of an Eisenstein series attached toclasses in
H*(~(0393BX), C)
or a residue ofsuch)
and whichrestricts isomorphically
under the restriction r* :H*(0393BX,C) ~ H*(~(0393BX), C)
onto the
image
of r*. This result leads to a direct sumdecomposition
ofthe
cohomology
of rwhere
H*!(0393BX,C)
denotes theimage
inH*(0393BX,C)
of the cohomol-ogy of
0393BX
withcompact supports
under the natural map. The spaceH*Eis(0393BX,C) decomposes naturally
as a direct sumwhere
H*max (resp. H*min)
is built upby
Eisensteincohomology
classesattached to
cuspidal
classes(cf. 3.1.)
on the facese’( P ) corresponding
tothe
r-conjugacy
classes of maximal(resp. minimal) parabolic
Q-sub-groups of G. _
However,
the actual construction of the classes inH*Eis(0393BX, C)
hasto be done on different
methodological
levelsdepending
on thetype
ofthe
cuspidal
class one’( P )
we start with. Forbuilding
upH4max(0393BX, C)
it is sufficient to consider each face
e’(P),
POE éP, /r, 1
=1, 2,
individu-ally ;
here 1 can availmyself
of thegeneral
results[22],
1concerning
theconstruction of Eisenstein classes in
this setting
and their restrictions to thecohomology
of the faces in~(0393BX).
But indealing
with the othercases 1 have to consider the faces
e’(P),
PE 3P,/r,
i =0, 1, 2,
simulta-neously,
and this canonly
be done in the adeliclanguage
in a satisfac-tory
manner. This ismostly
due to the fact that one has to take residues of Eisenstein series into account.Unfortunately,
theanalogue
of[22]
inthe adelic
setting
is notyet
at hand(but
inpreparation). Therefore,
1shall confine
myself
in this paper to construct in detailH4max(0393B; C)
(cf. §3). However,
for the convenience of thereader
1 shallbriefly
sketchin
§4
thecomplete
construction ofH*Eis(0393BX, C),
describe itsimage
under the restriction to the
cohomology
of theboundary
and indicate the ideas ofproof
in an adelicsetting.
1point
out that the methods used in§3 (cf. [22])
are sufficient to constructcompletely
the Eisensteincohomology H*Eis(0393BX, E )
if we aredealing
with a twisted coefficientsystem E given by
a finite dimensionalrepresentation
E ofSp4 (Q)
withsufficiently regular highest weight.
One has adecomposition
as in(3)
also for
H*(0393BX; ).
In both cases the results of§2
about the exactsize of the
cohomology
of r atinfinity
have to be used to obtain(3) (cf.
4.5.).
Conventions.
(1)
Thealgebraic
groups considered are linear and can be identified withalgebraic subgroups
of someGLn(C).
Wemainly
use thenotations in
[1].
For a(Zariski)-connected Q-group
H we denoteby
H =
H(R)
the group of realpoints
of H. An arithmeticsubgroup
of H is asubgroup
ofH(Q)
which is commensurable with03C8(H)~GLn(Z)
forsome
injective morphism 03C8: H ~ GLn
defined over Q. Weput ° H
=r1 ker X2
for a connectedQ-group
Hwhere X
runsthrough
the groupXQ(H)
ofQ-morphisms
from H toGLI ([3], 1.2.).
The group°H(R)
ofreal
points
contains each arithmeticsubgroups
of H and eachcompact subgroup
ofH(R).
(2)
Let M be a smoothmanifold,
and E a finite-dimensional vector space over C. ThenC’(M, E)
denotes the space of smooth functionswith values in
E,
and03A9q(M, E)
the space of smooth E-valued differen- tialq-forms
on M( q
=0, 1,... ).
Let9*(M, E )
be the direct sum of thegq(M, E )
endowed with exteriordifferentiation.
If E = C it will be omitted from thenotation;
thisapplies
also to the associated de Rhamcohomology
groups and thesingular cohomology
as well.(3)
We denoteby
A(resp. Af)
thering
of adeles(resp.
finiteadeles)
of the number field Q.
§1.
Preliminaries onSp4,
roots andparabolics
1.1. Let G be the
Q-split algebraic Q-group SP410,
i.e. thesymplectic
group of
degree
two. The groupG(R)
of realpoints
of G will be denotedby
G and we haveWe fix as maximal
compact subgroup
of G thegroup K
= G ~0(4),
i.e.the group of
orthogonal symplectic
matrices.Let P be a
parabolic subgroup
of G defined overQ,
N itsunipotent
radical and K: P -
P/N
= M the canonicalprojection.
Asplit
compo- nent of P =P(R)
isby
definition asubgroup
A of a Levisubgroup
of Psuch that A is
mapped isomorphically
via K onto theidentity component
of the groupSP(R)
whereSp
is the maximal centralQ-split
torus of M.By A p
we denote theunique split component
of P which is stable under the Cartan involution 0 associated to K. We then letM = ZG(Ap)
bethe
unique
O-stable Levisubgroup
ofP,
and we denoteby °M
theinverse
image
of0M(R)
under theisomorphism MP/N= M(R)
in-duced
by
K. We then have P = M. N as a semidirectproduct,
P =A p 0
Pand M =° M X
AP’
Since M isO-stable,
one has thatKp:=
K ~ P = K~0
M is a maximalcompact subgroup
of°M,
M and P.We fix the Cartan
subalgebra b
ofg = sP4(R)
formedby
the matricesand we
let 03A6 = 03A6 (gc, bc) be
the set of roots of g c withrespect to bc.
Its elements will also be viewed as roots of
Gc
withrespect
to H =ZG (b).
We choose an
ordering
on 03A6 in such a way that theweights of bc in
theorthogonal complement
p of f in g withrespect
to theKilling
form arepositive,
and denoteby à (resp. 03A6+)
the set ofsimple (resp. positive)
roots with
respect
to the chosenordering.
Then à=f al, 03B12},
where03B11(h)
=h1 - h 2
and«2 ( h )
=2h2
with hE 1)
as in(1).
TheWeyl
group W of gc withrespect to bc
is thengenerated by
thesimple reflections wl
associated to a,. We recall that we have
Since G is
split
over Q we may(and will) identify 4$ and 03A6R.
1.2. The set of
parabolic Q-subgroups
of G will be denotedby
.9. Theconjugacy
classes of elements in .9 areparametrized by
the subsets J of A. Inparticular,
ifQ
is a minimalparabolic Q-subgroup
ofG,
then it isconjugate
to the standard oneP = Po
whose
decomposition Po
°M0 · A0 · No
isgiven by
If
Q
is a maximalparabolic Q-subgroup
ofG,
then it isconjugate
to astandard one
given
as the semidirectproduct
of theunipotent
radicalby
the centralizer ofH0394-{03B11}, i = 1, 2,
where we denoteHj = (~03B1~J
ker03B1)0
c H for a subset J of 0394. Note that the characters of H inNi,
i =1, 2,
areexactly
thepositive
roots which contain at least onesimple
root notin à - (a,).
Theunique
0-stablesplit component
isgiven by
Since
MI
is the directproduct Sl2(R)
XGLI(R),
resp.M2;;; GL2(R)
wehave
The set of
simple
roots ofM,
=Z(Ai)
=Z(H0394-{03B1i})
isOMl
={03B1j},
i =Fj,
i, j = 1, 2.
Since
a
maximalparabolic Q-subgroup
P of G isconjugate
to itsopposite P,
the class%(P)
of maximalparabolic Q-subgroups Q
associ-ated to P coincides with the
conjugacy
class of P.(For
a definition of the notion "associate" we refer toII,
4[12].)
§2.
Theboundary
of the Borel-Serrecompactification
and itscohomology
2.1. Let r be a torsion free arithmetic
subgroup
ofG(Q)
=Sp4 (Q).
Thegroup r
operates properly
andfreely
on the associatedsymmetric
spaceX = G/K,
and thequotient 0393 B X
is a 6-dimensionalnon-compact K( r, l)-manifold
of finite volume. Thisquotient fBX
may be identified to the interior of acompact
manifold0393BX
with corners[3];
theinclusion 0393 B X - 0393 B is a homotopy equivalence.
Theboundary ~(0393 BX)
is adisjoint
union of a finite number of facese’(Q)
whichcorrespond bijectively
to ther-conjugacy
classes of properparabolic Q-subgroups
of G. For agiven
P in -9 with P = MAN as in 1.1. theprojection
K : P ~P/N
induces anisomorphsm
it: M -;P/N.
Weput
0393P = 0393~P
resp.0393N = 0393~N.
Then theprojection 0393M = k(0393P)
is anarithmetic
subgroup
ofPIN,
andKM = k(K ~ P) is a
maximalcompact subgroup
ofP/N
which isisomorphic
to K ~ M via jn. Thequotient Zm
=(0P/N)/KM
isagain
asymmetric
space which will also be viewedas
0M/K~M.
Then the facee’(P) corresponding
to ther-conjugacy
class of P is defined as
e’(P)
=0393pB0P/K
n P and it inherits from K afiber bundle structure
The fibers are
compact manifolds,
and the base space of the fibration may be identified with03BC-1(0393M)B0M/K~
M.If P is a maximal
parabolic 0-subgroups
of G oftype
i =1, 2,
thene’(P)
is a 5-dimensional manifold fibered over anon-compact
2-dimen- sional manifold0393MiBZMi (homeomorphic
to some arithmeticquotient
0393*iBSL2(R)/SO(2)) with
fiber a 3-dimensional nil-manifold for i = 1(resp.
torus for i =2).
If P is a minimal
parabolic 0-subgroups
of G oftype 0,
thene’( P )
=0393nBN
is a 4-dimensionalcompact
manifold which can be fibered in two different ways as a fiber bundle overS’.
For the standard oneP =
Po
these fibrationsfi, i = 1, 2,
are inducedby
theprojection
mapsof
No
onto theunipotent radical U
of the standard Borelsubgroup
of°Ml°,
and onegets
where
0393ui = 0393~Ui.
2.2. We now consider the full congruence
subgroup 0393(m) = {A ~ Sp4(Z) |A
= Idmod m }
ofSp4(Z)
for agiven m
3. We fix m once andfor all and will write r =
0393(m).
This alsojustifies
the notationfor the finite group, which
depends
on m. The groupSP4(Z) operates
ina natural way on the Borel-Serre
compactification 0393 B X
and so alsofG
acts on
H*(0393B)
resp.H*(~(0393BX)).
In a similar way the facese’( Pl ),
i =
0, 1,
2 are acted uponby Pi
~SP4(Z)
and weput
for i =0, 1,
2We have
0393(m)pi
=f(m)MI . 0393(m)Ni
in this case andfPi
is asplit
groupextension
of fMi by fNi.
Observe thatthe fPi
are ingeneral
notparabolic
subgroups
offG.
According
to[3]
there is a naturalcompactification Q
ofe’(Pi),
i
= 1, 2,
which adds over each cusp of the baseFMiB ZMi
a 4-dimensional nilmanifold. At the cuspcorresponding
to the(0393(m) ~0 Mi)-conjugacy
class of the standard Borel
subgroup
of0 Mio
this nilmanifold isexactly
the fibered manifold
f : e’(P0) ~ 0393UiBUi.
Inparticular,
the action ofPi
~Sp4(Z)
extends to one one’( Pi ), 1 and
the groupfPi
actstransitively
on the
boundary components
ofe’(Pi). Indeed,
one has anf Pi-equi-
variant
diffeomorphism
As
here,
we nowput
for i =0, 1,
2 resp. i =1,
2which is a
disjoint
union ofcopies
ofe’(Pi)
resp.Q
and has anatural action
of fG
which extends the oneof f Pi
one’(Pi)
resp.Q.
The
manifolds Y
arecompact
and one has anfG-equivariant
diffeomor-phism
defined
by
IdX 03B2i
onto theboundary ~(Yi). Using the ai
weget
a closed 5-dimensional manifold(with
an actionby fG)
by gluing together -
andY2 along
their common boundaries.By
thesame
arguments
as in[18], §6
one then obtains2.3. PROPOSITION:
The boundary ~(0393(m)BX) of
the Borel-Serre com-pactification r( m ) B X of r( m ) B
X isequivariant diffeomorph
with respectto the action
of fG
to themanifold
Ygiven
in2.2.(6).
2.4. In order to describe
H*(~(0393(m)B))
and to determine thefG-action
on this space we willanalyse
theMayer-Vietoris sequence
incohomology
attached to thedecomposition ~(0393(m)BX)
=Yl
UY2 .
Sincewe have as
f G-modules
(where IndÎpr [ ]
denotes therepresentation
offG
induced from therepresentation
offP,
onH*(e’(Pi)))
we will start with adescription
ofthe
cohomology H*(e’(Pi))
=H*(e’Pi))
asfPi-module.
We consider the fibration
0393Ni=Ni~e’(Pi)~0393MiBZMi
, fori = 1, 2
resp.
e’(P0) = 0393N0 B N0.
Thecohomology
of0393Ni B Ni
can be identifiedwith the
cohomology
of the Liealgebra
nof Ni.
Via this identificationH*(ni, C)
=H*(0393NiBNi) (cf. [22], 2.2.)
the naturalMi-module
structureon
H*(ni, C)
restricts to the action of0393Mi
onH*(0393MiBMi)
whichinherits therefore
by
extension a naturalMi-module
structure. If weput
then there is an
isomorphism
ofM;-modules ([13], 5.13)
due to Kostantwhere Fv
denotes an irreducibleMi,C-module
withhighest weight v E
(mi~b)*C
andl(w)
thelength
of an element in W. Oneeasily
checks(using
1.2. and1.1.(2))
Since
H*(e’(P0)) = H*(n0, C) decomposition (3) already
determinesH*(e’(P0))
asfP0-module.
Theunipotent
radicalNo operates trivially
onH*(n0, C),
so the actionof fP0
onFw(03C1)- 03C1 is given by
the action of thecommutative group
f Mo consisting
of four elements. Therefore for agiven
wFw(03C1)-03C1
contributes to thefP0-module H*(e’(P0))
as a one-di-mensional
representation (11w, F~w)
offPo
which is obtainedby
evaluat-ing w( p ) -
p onOMO,
hence onf Mo
andextending
ittrivially
tofN0,
i.e.we have as
¡Po-module
Associated to the fibration
2.1.(1)
of the facese’(Pi), i
=1, 2,
there isa
spectral
sequence which converges to thecohomology
ofe’(Pi),
andwhose
E2-term
isgiven by
Since the base space is of
type 0393’ B H ( H
= upper halfplane,
r’ cSL2(Z)
of finite
index)
andHp(0393’BH, ) = 0,
p >1,
for anarbitrary
coeffi-cient
system E
we haveEp,q2
= 0 for p >1, q
> 3 and thespectral
sequence
degenerates
atE2.
We obtainThe
M,-module
structure ofHq(ni, C)
iseasily
determinedby
means of2.4.(3). One gets
2.5. PROPOSITION: The
cohomology H*(e’(Pi)) of
theface e’(Pi),
i =1, 2,
is
given
as¡P¡-module by
If we denote by Ek(i)
resp.E03C3k(i)
the k-dimensional irreducible representa- tionof 0Mi
with0M1 ~ SL2(R) x {±1}
and0M2 ~ SL2± (R ) = Sl2(R){±1}
where(-1)
operatestrivially
resp.non-trivially
then wehave
the following isomorphisms of 0 Ml-modules:
The action
of fPl
onHP ( f MI B ZMi, Hq(ni, C))
is thepullback of
the actionof ¡Mi
on thesecohomology
spaces obtainedby
the natural actionof
°M,
~SP4(Z)
onfMIBZMI
resp. the action onHq(ni, C) just
described.2.6. In order to determine
H*(~(0393(m)BX))
we nowstudy
the kernelresp. cokernel of the
morphism ai
~03B1*2
in theMayer-Vietoris
sequenceattached to
the decomposition ~(0393B ) = 1 ~ Y2 of
theboundary.
Since
~(0393B)
is connected weget
fordegree
0by 2.4.(1)
and(5)
resp.2.5. the
following
short exact sequence offG-modules
The
fG-module coker(03B101 ~ a2)
isuniquely
determinedby (2)
and will be denoted(analogue
theSteinberg module) by St(m).
Before we consider the situation in
degree
1 we recall that the spacee’( Po )
=fNo BNo
can be fibered in two different ways(2.1.(3))
The associated
spectral
sequence written in Liealgebra cohomology
terms
degenerates
atE2.
This is a consequence of Kostants result(cf. 2.4.(3)),
for
example.
We now consider the
morphism
indegree
1(using 2.4.(1)
and2.5.)
where the
right
hand side is also a sum of two termsby 2.4.(3)-(5). By
ananalysis
of the¡P¡-module
structure on both sidesgiven
in2.4.(5)
resp.2.5. and
(3)
it turns out that03B111 ~ 03B112
is the sum of the twofG-morphisms
induced from the
¡P¡-morphisms
By
construction this isexactly
the restriction map ofH1(0393Mi B i)
to thecohomology
of theboundary of the
base space0393Mi B Zi.
Since as avectorspace H2(0393Mi B Mi, ~(0393MiBZMi))~C
the cokernel of this restric- tion is a onedimensionalreprésentation [rj ]
offP, .
The kernelis,
ofcourse, the
image
of thecohomology
withcompact support
offM BZM
and can be identified with the cusp
cohomology H1cusp(0393MiBZMi) (cf.
3.1.or
[2]
5.5 fordefinition).
Therefore we have a short exact sequence offPi-modules
and we obtain
where the action
of fPi
onH1cusp(0393MiBZmi) is
thepullback
of the naturalaction of
fMi
on the cuspcohomology.
The situation in
degree
2 isquite
similar to theprevious
case.By 2.4.(1)
and 2.5. we have to considerThen
again using (3), 2.4.(5)
and 2.5. thismorphism
is the sum of the twofG-hornomorphisms
induced from thef Pi-morphisms
The
right hand side
is thecohomology
of theboundary
of thecompacti-
fication
0393Mi B ZMi
of the base space. SinceH1 (ni)
is not the trivialMi-module C (resp. C03C3) (cf. 2.5.)
this map issurjective
and determinedby
the short exact sequence offPi-modules
This
implies
These
investigations
indegrees 0, 1, 2
allow usalready
to determinecompletely
thefG-module H*(~(0393B)).
For . later purposes wegive
adescription
of thecohomology
which reflects thegeometric
source of thevarious summands.
2.7. THEOREM: For a
given
congruencesubgroup f
=0393(m) of SP4(Z),
m
3,
thecohomology of
theboundary ~(0393(m)B) of
the Borel-Serrecompactification of 0393(m) B
X is described asrepresentation
spaceof fG
=Sp4(Z/mZ) by
( For
notation resp. adescription of
theMi-module
structureof Hq(ni)
andthe action
of fPi
on the various termsHpcusp(0393Mi B ZMi, Hq(ni))
werefer
to2.5.)
ThefG-module St(m)
isdefined by
the short exact sequenceThe
boundary ~(0393(m)BX)
is acompact
connected 5-dimensional manifold.By Poincaré-duality
thisimplies (1).
Assertion(2) (resp. (3))
follows from
2.6.(1), (7) (resp. 2.6.(11), (8)). Again, by Poincaré-duality (2) (resp. (3))
and 2.5 thenimply
also(5)
and(4). Indeed, by determining
kernel and cokernel of
ai
~a*
also indegree
3 and 4 as above these lasttwo statements can also be seen
directly.
Inparticular,
one checksby
2.5.that the 1-dimensional
representation H0(0393Mi B ZMi, H3(ni)) of fPi
cor-responds
to[03C4i].
2.8. In view of this result there are some observations of interest
concerning
the natural restrictionIt is clear that
r0
is anisomorphism.
Thepositive
solution of thecongruence
subgroup problem
forSp4 (cf. [19])
shows that the commuta-torfactorgroup r/[r : ] ]
is finite. On onehand,
thisimplies
thatH1(0393BX)=0393/[0393:0393]~C
vanishes and viaPoincaré-duality
onegets
that
r4
issurjective.
On the otherhand,
one obtainsH1(0393B)
=0,
andtherefore r’
is trivial.Moreover,
there is a dualpairing
onH*(~(0393B))
induced
by duality (cf. [5],
p.305)
such that theimage
ofH*(0393B)
under r * is its own
annihilator;
inparticular
onegets
for i =0, 1, ...
which shows that
Im r 3
andlm r 2are
related to eachother.We now consider the congruence
subgroup 0393(m),
m 3. ThenrMJ
can be viewed as the full congruence
subgroup r(2, m)
of level m inSL2(Z).
The Eichler-Shimuraisomorphism (cf. [25], 8.2)
relates the cusp
cohomology
ofr(2, m )
with coefficients in the represen- tation ofSL2(R)
of dimension k to the spaceSk+1(0393(2, m ))
of holo-morphic
resp.antiholomorphic cuspidal
forms ofweight
k + 1 on theupper half
plane H
withrespect
tor(2, m ).
The dimension of the spaceson the
right
hand side are known([25], §2). Using
this and(2)
we obtainthe
following
dimension formulas for theimage
of the restriction map r*.2.9. PROPOSITION: Let r =
r( m ),
m3,
be the congruencesubgroup of
level m
of SP4(Z).
Thedimensions of
theimages of
the restrictions r*:H*(0393B)~ H( 8 ( r N X))
aregiven by
where
pj ( m ) = |fPjBf G |
denotes the numberof 0393(m)-conjugacy
classesof parabolic 0-subgroups of SP4(R) of type j ( j
=0, 1, 2).
§3.
Eisensteincohomology 1
We will now use
the theory
ofEisenstein
series([12], [15])
to construct asubspace H4max(0393B)
inH4(0393 B )
which isgenerated by regular
Eisen-stein
cohomology
classes and which restrictsisomorphically
onto thecuspidal cohomology
of the facese’(Q) where Q
runsthrough
a set ofrepresentatives
for the maximalparabolic Q-subgroups
of G moduloconjugation by
r(3.3., 3.4.).
We assume somefamiliarity
with the results in[22],
I. The other cases will be dealt with in§4.
3.1. Eisenstein series. Given a
parabolic 0-subgroups
P of G withP ° MAN
thecohomology
of thecorresponding
facee’(P)
in theboundary
of the Borel-Serrecompactification 0393 B X
offBX
isgiven
as(cf. 2.5.)
It contains as a natural
subspace
the cuspcohomology
of
e’( P ). By
definition([2],
5.5 or[22], 1.6),
thissubspace
isusually
viewed in terms of relative Lie
algebra cohomology
as theimage
of theinjective homomorphism
Here
L20(0393MB0M)~
denotes the(om, KM)-module
of C’-vectors in therepresentation
spaceL20(0393MB0M)
ofcuspidal square-integrable
functionson
0393MB0M
acted uponby °M
viaright
translations. For the notion of relative Liealgebra cohomology
we refer to[4],
I.However,
thissubspace
may also be
interpreted
in terms ofH*(n)-valued
differential forms whose coefficients areH*(n)-valued cuspidal
functions. Inparticular,
the cusp
cohomology H*cusp(e’(P))
can be identified with the space of harmoniccuspidal
C-valued differential forms one’(P),
i.e. thosewhosè
coefficients are
cuspidal (see [2], §5).
Let 0 ~
[~] ~ H*cusp(e’(P)) be a
non-trivialcuspidal cohomology
classrepresented by
a harmoniccuspidal form 0
E03A9*(e’(P)).
Recall that wehave
topologically 0393PBX=e’(P)xAp.
For agiven A E ût
we canassociate
to ~
via the differential form~039B= ~a039B+03C1
in03A9*(0393P B X)
theEisenstein series
(cf. [22], §4)
This Eisenstein series is first defined for all A in
and is
holomorphic
in that tube where0394(P, A )
denotes the set ofsimple
roots of P with
respect
to A and the element03C1P ~ a*
is definedby
03C1P(a)=(det Ada |n)1/2,
a ~ A . Viaanalytic
continuation it admits ameromorphic
extension to all ofa*C.
We refer to[12], [15]
for thegeneral theory
of Eisenstein series. If039B0 ~ at
is fixed andE«p, A)
is holomor-phic
at thispoint,
thenevaluating
the Eisenstein series inAo gives
aC-valued,
r-invariant differential formon X,
i.e. we obtainE(~, Ao) EE 03A9*(0393 B X).
Infact, by
4.11[22]
there is aspecial point 039B~ uniquely
determined
by ~
such that this constructionprovides
us with a closedharmonic form
E(~, 039B~)
ifE(~, 039B)
isholomorphic
at thispoint Acp.
Inparticular,
this formrepresents
a non-trivialcohomology
class[E (~, 039B~)]
in
H*(rBX).
3.2. We now assume that P ° MAN is a maximal
parabolic
0-sub-group of G. The space
L20(0393MB0M) of
squareintegrable cuspidal
func-tions on
0393MB0M decomposes
into a direct Hilbert sum of closed irreduci- ble°M-invariant subspaces H03C0
with finitemultiplicities m(03C0, 0393M) ([12],
1.
§2).
IfVTT
denotes theisotopic component
of 03C0~0 M
we may writeBy
definition of the cuspcohomology, 2.4.(3)
and[22] 1.6
we then have afinite sum
decomposition
Now,
the irreducibleunitary representations
of°M
which may contrib- utenon-trivially
for a fixed w ~W p
to theright
hand side are well-known.Let
Fk
=Ek (resp. Et)
as in 2.5. a k-dimensional irreduciblerepresenta-
tion of0 M,
which isisomorphic
toSl2(R)x(±1)
for i = 1 resp. toSL2±(R)
for i =2,
and we assume k > 1 for the moment. If(03C0, H03C0)
isthen an irreducible
unitary representation
of0 Mi
which is notequivalent
to a discrete series
representation D± 1
for i = 1(resp. Dk+1
for i =2)
of lowest
KMi-type
k + 1(cf. [27], 1, §4)
we haveand for the discrete series
representations D±k+1
1 resp.Dk+1
we havewith irk,l
= D±k+1
f or i = 1(resp. = Dk+1 for
i =2).
This formula holdsalso for k = 1
(i.e. F1 = C or C03C3).
But in this case also the trivialrepresentation C resp. Ca
contributenon-trivially
indegree
0(resp. 2).
For all other
representations non-equivalent
to these three ones there isagain
avanishing
result as in(3). By
means of 2.5. theright
hand side of(2)
then reduces for a fixed w EW’
oflength l(w)
withFw(03C1)-03C1 ~ Fk
toWe
observe,
that thisreflects,
more orless,
in arepresentation
theoreti-cal version the Eichler-Shimura
isomorphism (cf. 2.8.).
Inparticular,
forr =
1’(m)
themultiplicity m(DkI, 0393M)
isgiven
as the dimension of the spaceSk(r(2, m))
of cusp forms withrespect
tor(2, m)
cSL2(Z)
ofweight
k in the classical sense.We will now discuss the use of Eisenstein series associated to cusp forms in
H4cusp (e’(P))
to constructcohomology
classes inH4(0393 B X).
Asa final
result,
we will obtain acomplete description
of thecohomological contribution
toH4(0393 B X) by
the cuspcohomology
of the faces in~(0393 B X)
of minimal codimension. To deal with thisproblem
in thedegrees
2 and 3 deserves a differentapproach (cf. §4).
3.3. THEOREM: Let r c
SP4(Z)
be a torsionfree subgroup of finite index;
let P be a
maximal parabolic Q-subgroup of Sp4(R). If [~] ~ H*cusp(e’(P))
is a non-trivial
cuspidal cohomology
classof degree
4 then the Eisenstein seriesE (~, A),
039B Ea t,
associated to[~] ]
isholomorphic
at thepoint
Acp = - wp(p) |a
= p p( uniquely
determinedby ~).
Theform E (~, 039B~)
isclosed
and
harmonic and represents anon-trivial
class inH4(0393 B X )
whoseimage
under the restrictionrJ: H*(0393 B X) ~ H*(e’(Q))
to aface e’(Q)
in~(0393 B X)
isgiven by
PROOF: We can assume that P is standard. For the cusp
cohomology
ofthe face
e’( P )
indegree
4 we haveby
2.5. resp. 3.2.with
H3(ni)
=FwP(03C1)-03C1
where wp denotes thelongest
element inWP,
andsince
FwP(03C1)-03C1 ~ C resp. C °
as°M-module
weget
i.e. the non-trivial class
[~] is necessarily
oftype (03C02, wp )
in the sense of3.2.
[22].
Thespecial point 039B~ uniquely
determinedby ~
is thengiven
asit lies outside the tube
(a*C)+
of absolute convergence of the associated Eisenstein seriesE(o, A). However,
since 03C02 is atempered representa-
tion the result6.4.(2) [22] applies
andE(~, A)
isholomorphic
at039B~. By
4.11.
[22],
the formE(~, 039B~)
is closed and harmonic andrepresents
a non-trivial class[E(~, 039B~)]
inH4(0393BX).
We recall that the
image
of[E(~, 039B~)]
under the restrictionrQ*
isgiven
as[E(~, 039B~)Q]| e’(Q)
i. e.equal
to the restriction toe’(Q)
of theclass
[E(~, 039B~)Q] ] represented by
the constant Fourier coefficientE(~, 039B~)Q~03A9*(0393Q B X)
ofE(~, Acp) along Q ([22], 1.10).
Thetheory
of the constant term
(cf. [12], II, 4., 5., [22], 4.7.)
thenimplies
thatE(~, 039B~)Q
vanishes ifQ
is not associated to P. Since this condition is in this caseequivalent
to the factthat Q
is notG(Q)-conjugate
to P weobtain
If
Q
is associated to P thenby
definition the finite setW(Ap, AQ )
ofisomorphisms
ofA p
ontoAQ
inducedby
innerautomorphisms
of Gdefining a Q-isomorphism
ofMP(R)
ontoMQ(R)
is notempty;
we havewhere
c(s, 039B~)s039B~: 03A9*(0393P B X) ~ 03A9*(0393Q B X)
is an"intertwining"
oper- ator defined in 4.10.[22].
As
pointed
out in 1.2. the maximalparabolic
P isconjugate
to itsopposite
P. Thisimplies
inparticular
that the setW(Ap, AP)
consists of two elements. If weput
then we have
(in
the notationAl
=AP )
Since a maximal
parabolic Q-subgroup Q
in the associated class&(P)
of P is
conjugate
toP,
there is an elementg E G(Q)
with P g =Q,
andAQ
=A5
is asplit component
ofQ.
We then obtainWe now deal with the case
that Q
isr-conjugate
to P.By 7.7.(1) [3]
wethen have
e’(P) = e’(Q)
and we can assume P =Q.
The summand in thesum
(6) corresponding
to the element 1 inW(Ai, Ai)
then contributesby
the class
[~] we
started with(cf. 4.9., 4.12(6)
in[22]).
The other summand[c(s" 039B~)si039B~(~039B~)]| e’(P)
in(6)
is acohomology
class inH*cusp(e’(P))
ofweight vsi(p)-p|ai (in the
sense of[22], 3.2.) where vs@
is auniquely
determined element in
W
withvs/p) 1 al +si039B~ = 0 (and
a secondcondition not of interest
here,
cf.[22], 4.10.(11));
thatis,
this class is contained inH1cusp(0393MBZM; Fvsi(03C1)-03C1).
Sincesi039B~ = -039B~
this condition isequivalent
toand one sees
that vsi
= 1 EWp,.
Since this occursonly
indegree
1 inH*cusp(e’(Pi)) (cf. 2.5.)
this second summand(indeed,
therepresenting
differential
form)
vanishes. So we haveWe now assume
that Q in &(P)
is notf-conjugate
toP,
and we writes for the element Int
g 1 Ar
in(9). By
definition(4.8. [22])
theoperator c(s, Acp)sA.p
isgiven
as a sum over terms which areparametrized by
theset
r(s )
= F nPg-’Q.
For an element y =pg-Iq
in0393(s),
p EP,
q EQ,
we have
y -1Py = q-1gp-1Ppg-1q
=Q;
but this contradicts our assump- tionthat Q
is notr-conjugate
toP,
and therefore we have thatr(s)
isempty.
Indealing
with the second summand in(6)
one observes as abovethat it has a
weight
which does not occur indegree
4 of[E(~, 039B~)].
Sowe
finally get
3.4. COROLLARY: Let P be a maximal
parabolic 0-subgroup of G,
andlet
W (P)
be its associate classof parabolic Q-subgroups.
LetHi(p)(fBX)
be the
subspace
inH4(0393 B X )
which isgenerated by
the Eisenstein cohomol- ogy classes[E(~, 039B~)]
constructed as in 3.3.for
all R in a setof representatives of 0393 B &(P)
and all non-trivial classes[~] ~ H4cusp(e’(R)).
Then