C OMPOSITIO M ATHEMATICA
J ÜRG K RAMER
A geometrical approach to the theory of Jacobi forms
Compositio Mathematica, tome 79, n
o1 (1991), p. 1-19
<http://www.numdam.org/item?id=CM_1991__79_1_1_0>
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A geometrical approach
tothe theory of Jacobi forms
JÜRG
KRAMERDepartment of Mathematics, ETH-Zentrum, CH-8092 Zürich, Switzerland Received 21 September 1989; accepted 11 July 1990
(Ç)
Introduction
In this note we
give
ageometrical approach
to thetheory
of Jacobiforms,
whichwas
originated
in ananalytic
wayby
Eichler andZagier (cf. [4]).
There Jacobiforms are introduced as
holomorphic
functions on e x C(~:
upper half-plane) satisfying
a certain transformation law withrespect
to the semi-directproduct
0393Z2 (I-’: subgroup
of finite index inSL2(Z»
andhaving distinguished
Fourier
expansions
at the cusps.We start in the first section
by recalling
some basic facts about theelliptic
modular surface
Xr
associated to rfollowing
the article[9].
Tosimplify
theexposition,
we restrict ourselves to the cases, where r acts without fixedpoints.
In the second
section,
we characterize the space of Jacobi cusp formsof weight ke2N,
index m ~ N withrespect
to r as the space ofglobal
sections of adistinguished
subsheafFk,m
of a certain line bundleOX0393(Dk,m)
onXr.
In the third
section,
we prove theampleness
of the line bundle(9x,(Dk,.)
fork,
mbeing large enough. By using
the Riemann-Roch Theorem for the surfaceXr,
we then determine the dimension ofHO(Xr, OX0393(Dk,m)). By proving
thevanishing of H1(X0393,Fk,m),
we arefinally
inposition
to derive a formula for thedimension of the space of Jacobi cusp
forms,
which can be made moreexplicit
under the extra
hypothesis
that the least commonmultiple
of all the cusp widths divides m. Formulas for the dimension of the space of Jacobi cusp forms werealready
obtained for r =SL2(Z), r o(p) (p
aprime) by analytic
methods in[4], [6]
and in fullgenerality, by using
a trace formula for Jacobi-Heckeoperators (cf. [11]),
in thepreprint [10].
Our final formula is identical with the onegiven by Skoruppa
in[10].
1. Notations and Definitions
Let 0393 be a
subgroup
of finite index inSL2(Z)
and Jf the upperhalf-plane.
Assume that r acts without fixed
points and -1 ~
0393.Let Yr be
the modularcurve associated to
r,
i.e. thecompactification
ofrBJf by adding
the cusps.Denote
by
u, the number of cusps andby nj
the cusp width ofthe jth
cuspAssume furthermore that
Yr
has no cusps of the second kind.Denote
by X r
theelliptic
modular surface associated tor, by
n :X0393 ~ Yr
thenatural
projection
andby
0":Yr - Xr
the zero section. From[5], §8
or[9],
PartII,
we know thefollowing:
Because of ourassumption
onr,
theonly singular
fibres of n lie above the 6r cusps of
Yr;
these arenj-gons,
i.e.where
~j,v ~ pl
is embedded intoX r
with self-intersectionnumber - 2,
and otherwise(here
andbelow, v,
v’ have to be understood modulonj).
In terms of local coordinates the situation above the cusp
Pj
can be describedas follows:
j,v
cXr
can be coveredby
two affine chartsUj?v, W1j,v
cXr,
wherethe coordinates
uj,v, vj,v
ofWjov
can be chosen such thatj,v|w0j,v
isgiven by
theequation vj,v
= 0(uj,v-axis)
and hence the coordinates ofW1j,v
areu-1j,v, u2j,vvj,v
(note
that0398j,v. 0398j,v = -2).
Because0398j,v+1
and0398j,v
intersecttransversally,
wededuce from this the
following
relationsFurthermore we note
with q. =
e203C0iM-1j03C4/nj, 03BEj
=e2niz/( -Cj!
+ aj)(03C4
EJf ZEe)
By
gr resp. Pa we denote the genus ofYr
resp. the arithmetic genus ofX r.
Wehave the formulae
(cf. [5], §12
or[9],
pp.35-36)
Finally,
we denoteby KY0393
resp.KXr
the canonical divisor ofYr
resp.Xr.
2. Geometrical characterization of Jacobi forms
Let k ~ 2N and m~N. From
[4],
we recall thefollowing
DEFINITION 2.1. A
holomorphic
functionf:Jf
x C - C is called Jacobi cuspform of weight k,
index m with respect tor,
if it satisfies thefollowing properties:
(ii)
At the cuspPj ( j
=1, ... , 6r), f
has a Fourierexpansion
of the formThe
C-span
of these functions is denotedby Jcuspk,m(0393).
We are now
going
to describe the elements ofJcuspk,m(0393)
asdistinguished
sections of a certain line bundle over
Xr.
Weput Y00393:=0393BH
andXI:= 0393Z2BH
x C. We make thefollowing
observation: It isimmediately
checked that
define two
1-cocycles,
whence two1-cohomology
classes yl, y2 resp. ofH1(0393Z2, C*) ~ H1(X00393, (9*o - Pic(Xr) (cf. [7], Appendix
to1.2).
The classicaltheory
of modular forms shows that theisomorphism
class inPic(X’)
corre-sponding
to y 1 can berepresented by
the line bundleNow let
[2]
be theisomorphism
class inPic(X’) corresponding
to y2.By restricting [2]
to anarbitrary
fibreEt
of ri Eyro,
we obtain anisomorphism
class of line bundles on the
elliptic
curveE,.
Thecorresponding 1-cohomology
class
of H1(E03C4, O*E03C4) ~ H1(, C*) (where
A is the lattice Z03C4 Ef)Z)
is determinedby
the
1-cocycle
One checks that this
1-cocyle
differsonly by
a1-coboundary
from the1-cocyle
defined
by
where
By
the theorem ofAppel-Humbert,
we find that[2] lE.
=L(H, 1) (cf. [7],
p.
20)
and therefore can berepresented by OE03C4(2m · O),
where 0 denotes theorigin
of
E,.
Hence[Y]
can berepresented by
the line bundleOX0393(2m03C3(Y0393))|X00393. (2)
The
problem
now consists infinding appropriate
extensions of the line bundles(1), (2)
to the whole ofXr.
To solveit,
we determine the divisor of asuitably
chosen
(meromorphic)
Jacobi form ofweight k,
index m withrespect
to r.We first recall two
elementary
lemmas.LEMMA 2.2. The
theta function
satisfies
thefunctional equation
LEMMA 2.3. The eta
function
satisfies the functional equation
We
put
x:=(X1X2l)2m
and denoteby (9Y,(Mk,î)
the line bundle associated toholomorphic
modular forms ofweight k
and character~
withrespect
tor;
itsdegree
isgiven by k03BC/12.
Forexample,
for X =1,
we havePROPOSITION 2.4. For any
f
EJcuspk,m(0393),
we havewhere - means linear
equivalence of divisors.
Proof.
Let g be anyholomorphic
modular form ofweight
k and character~
with
respect
to r andput
By
construction we haveTo
complete
theproof,
we have tocompute div 0 1, 1
anddiv ~.
Theonly
non-trivial
part
of this calculation is the determination of themultiplicities of 01,1
onthe
components 0398j,v:
From the Fourierexpansion
of01,1
we obtainhence the
multiplicity
of61 .
on8i.v equals
Summing
up, weget
as claimed.
THEOREM 2.5. The
map f -
divf
induces aninjection
where
(Ilxll ~ meaning
the distanceof x
to the nearestinteger
and[x]
thegreatest integer
~ x).
Proof.
Letf
EJcuspk,m(0393). By
definition divlx-
iseffective;
therefore it remainsto determine the
multiplicities of f
on thecomponents 8j.v: By
Definiton2.1(ii),
we obtain
hence the
multiplicity
off
on0398j,v
isbigger
orequal
toFrom
Proposition
2.4 and the abovecomputation
weget
This
completes
theproof
of Theorem 2.5. DTo describe the
subspace
im i gH°(Xr, (9x,(Dk,.» corresponding
to the spaceJcuspk,m(0393),
we have to introduce some definitions:For
x~R,
denoteby x
the nearestinteger
of x.For j
=1,
... , 6r andv =
0, ... , nj -
1 defineintegers v- 0, v + 0 satisfying
theproperties (i)
theintegers
in the intervalform a
complete
set ofrepresentatives
of the residue classes modulo2m,
is minimal.
Finally,
define the subsheaf197k,.
of(9x,(Dk,,,,)
to consist of those sections shaving
theproperty
that in theirTaylor expansions
on
Woj,v,
i.e. around the verticesQj,v: = 0398j,v-1 ~0398j,v
of thenj-gons 03C0-1(Rj),
thecoefficients
bj,v(k, l)
vanish forwhere
03C1:= k -
1 +03B2j,v+1
-03B2j,v
isrunning
from( j
=1, ... ,
6r; v =0, ... , nj - 1).
We note thatFk,m
is not an(9x,-submodule
ofOX0393(Dk,m)
ingeneral.
With these definitions we prove THEOREM 2.6. There is an
isomorphism
Proof.
Lets ~ H0(X0393, (9x,(D,,.»
be aglobal
sectionbelonging
to im 1. Fromthe
proof
of Theorem 2.5 we know that the Fourierexpansion
at the cuspPj
ofthe Jacobi form
corresponding
to s is obtainedby taking
one of theTaylor expansions (3)
of s(around
the vertices6;, y), multiplying
itby u03B2j,vj,v+1v03B2j,vj,v
and
substituting
uj,v, vj,vby qj-v03BEj, qv+1j03BE-1j respectively; putting
p:=k-l+03B2j,v+1-03B2j,v,
we find the Fourierexpansion
The above
analysis
shows: SE im 1, if andonly
if the coefficientsbj,v(k, 1)
in theTaylor expansions (3)
vanish for(j=1,...,03C30393; v=0,...,nj-1).
The number of the conditions(5)
can now beminimized as follows:
By
theargument
of[4],
p.23,
we know that(5)
has to befulfilled
only
for prunning through
acomplete
set ofrepresentatives
of theresidue classes modulo 2m.
Observing
thatthe nj Taylor expansions (3)
aroundthe vertices
Qj, 0, . - - , Qj,nj-1
determine the Fourierexpansion
of thecorrespond- ing
Jacobi form at the cuspPj,
weoptimize
theproblem by distributing
theconditions
(5)
in a minimal way amongthe nj Taylor expansions (3). Recalling
the definitions
preceding
Theorem2.6,
we see that theoptimal
result is achievedby imposing
at each vertexQj,v
the conditionsbj,,(k, 4
= 0 forwhere p is
running
fromi.e., s c- im 1,
if andonly
ifs ~ H0(X0393, 57k,.)-
REMARK 2.7. From
inequality (4)
and the estimatewe note that the number
Cj
of conditions for each cuspPj,
which define thesheaf
Fk,m
as a subsheaf ofOX0393(Dk,m),
isgiven by
the formula3. Dimension
computations
To
compute
dimH°(Xr, OX0393(Dk,m))
and dimH0(X0393, Fk,m),
we need thefollowing
LEMMA 3.1.
Define 03B1j,v and 7j,v by
for j =1, ... ,
a, andv = 0,
...,nj-1,
extended to all v E 7Lby periodicity
in v withperiod
nj, andProof.
The case m = njbeing easily
treatedby
directcomputation,
we assumefrom now on m > n;. With
0
p;_v1, (7) equals
Introducing
thepolynomial Pj (v): = - mv(nj - v)/nj+mnj/6-1
andÂj: = 2m/nj,
we can rewrite
(8)
asObserving
Noting
that for all real x andwhich
by periodicity
also holds for all real xand 03BE,
we obtain(by taking x=03BBj-2 and 03BE=03BBjv)
This
completes
theproof
of the lemma. r-iPROPOSITION 3.2.
If k
m + 4 and m nj(all j),
the line bundlelPxr(Dk.m - KXr)
isample.
Proof.
We have(cf.
Theorem 2.5 and(7))
By
the criterion ofNakai-Moishezon,
we have to show that the intersection numbers ofDk,m - KX0393
with all irreducible curves C cX r
arepositive.
Wedistinguish
thefollowing
three cases:C =
E,
aregular
fibre of n, i.e. anelliptic
curveC =
0398j,v (all j, v)
C is a horizontal
divisor, i.e., 03C0(C)
=Yr.
In the first case, we have
In the second case, we have
by
Lemma 3.1Before
treating
the last case, we recall from[5], §12
thatKXr=n*(KYr-F)
with
F E Div( Yr), deg F = - pa -1;
with theadjunction
formula we thereforeobtain
For the last case we
distinguish
C =6(Yr)
andC ~ a(Yr).
In the firstsubcase,
wehave
The formulae for the genus gr and the arithmetic genus pa
given
in the firstsection and the relation Jlr
= 03A3jnj
nowimply
For the second
subcase,
we first note that8j.v.
Cequals
zero for all but one v =:vj, where we have0398j,vj.
C = 1. We now obtain the estimateThis finishes the
proof
of theproposition.
THEOREM 3.3.
If k
m + 4 and m nj(all j),
we have thedimension formula
Proof. By Proposition
3.2 the line bundlelPxr(Dk.m - Kxr)
isample
andtherefore we have
by
the KodairaVanishing
Theoremdim
H1(X0393, OX0393(Dk,m)) =
dimH2(X0393, (9x,(Dk,.» =
0.Now we obtain
by
the Riemann-Roch TheoremWe denote
by k,m
thequotient
sheafOX0393(Dk,m)/Fk,m.
It is askyscraper
sheafsupported
on the verticesQj.v
of thenj-gons 03C0-1(Pj). By
definition we havewith
Cj given by (6).
We are now able to proveTHEOREM 3.4.
If
k » 0 and m nj(all j),
we have the dimensionformula
Proof.
Consider the exact sequence of sheavesIf we are able to show
H1(X0393, Fk,m)
={0},
thelong
exact sequence incohomology
associated to(10) implies
The claim then follows
immediately
from Theorems2.6,
3.3 and formula(9).
We are left to show
H1(X0393, Fk,m)
={0}.
This will be done in twosteps:
lst step. We introduce an
auxiliary
subsheafF’k,m
ofFk,m
as follows: With03C1(±):= v(±)
-2mv/nj put
Define the
OX0393-submodule F’k,m
ofOX0393(Dk,m)
to consist of those sections shaving
the
property
that in theirTaylor expansions (3)
around the verticesQj,v
of the nj-gons 03C0-1(Pj),
the coefficientsbj,v(k, l)
vanish for( j
=1,...,
03C30393; v =0,..., nj - 1). By
constructionF’k,m
is a subsheaf ofFk,m
andthe
quotient OX0393(Dk,m)/F’k,m
isagain
askyscraper
sheaf’k,m supported
on thevertices
QJ,y.
We have thefollowing
exact sequences of sheavesThe first
part
of thelong
exact sequence incohomology
associated to(11)
leadsto the
diagram
From
(12)
weeasily
derive thatH1(X0393, F’k,m) = {0} implies H1(X0393, Fk,m)
={0}.
2nd step. To prove the
vanishing
ofH1(X0393, F’k,m),
we introduce theauxiliary
line bundle
L’k,m:= OX0393(D’k,m)
withFrom the exact sequence of
(9x,-modules
we deduce that the
vanishing
ofH1(X0393, L’k,m)
andH1(X0393, L’k,m) implies
thetriviality
ofH1(X0393, F’k,m).
Thevanishing
ofH1(X0393, L’k,m)
follows from theampleness
of the line bundleUxr(Dk,m - Kxr)
for kbeing large enough,
which isproved along
the same lines asProposition 3.2;
a crude estimate showsTo prove
H1(Xr, ’k,m)
={0},
we note(after
a shortcalculation)
that thequotient L’k,m = F’k,m/L’k,m
isisomorphic
towhence
because
0398j,v ~ pl
has self-intersection number - 2 andhi
> 0(all j).
Thisfinishes the
proof
of the theorem. DFrom Theorem 3.4 we are able to deduce an
explicit
formula for dimJcuspk,m(0393) assuming k
» 0and nj|m (all j).
To dothis,
we use aslight generalization
of thelemma
proved
in[4],
p. 124.Actually,
we will prove a little more than wefinally
need. As in
[4]
we introduce the functionLEMMA 3.5. For
positive integers
n,N,
we havethe formula
where
H(A)
denotes the Hurwitz classnumber,
i.e. the(weighted)
numberof SL2(Z) equivalence
classesof
allpositive definite, integral, binary quadratic forms of
discriminant A.
Proof.
First suppose(n, N)
= 1 and N is aprime. Then,
as in[4],
p.124,
we observe that the cases N = 2 and N - 1 mod . 4 aretrivial;
in the case N ~ 3mod . 4,
we obtain for the left-hand side of(13)
by
thequadratic reciprocity
law and Dirichlet’s class number formula. The caseof
composite
N and(n, N)
= 1 is then treatedfollowing
the sketchgiven
in[4], nx2
p. 125. To prove
(13)
in thegeneral
case, we observe that thefunction N
isperiodic
in K withperiod N/(n, N);
thisgives
Now formula
(13)
follows from thepreceding
case.LEMMA 3.6. For m, nj as
above,
thefollowing formula
holdswhere
Q(N)
denotes thelargest integer,
whose square divides N.Proof. Applying
Lemma 3.5 with n = nj and N =4m,
we obtainObserving
that the functionn’x 2
isperiodic
in K withperiod 2m/(m, nj),
wecan rewrite the left-hand side of
(14)
toA short calculation shows that this
equals
which
completes
theproof
of the lemma.Finally,
we needLEMMA 3.7.
If nj|m,
we haveProof.
We haveand, by symmetry,
for v =
0,...,
nj - 1. Therefore we havemax(O, -
p +/3j.V+
1 -/3j.v)
= 0 for prunning
from v - -2mv/nj,..., v+ - 2mv/nj,
and we obtainWe now prove
THEOREM 3.8.
If
k » 0 andnj| m (all j),
we have the dimensionformula
Proof. Because nj|m (all j),
we havewhence
By
Theorem 3.4 and Lemma3.7,
we then obtainUsing
Lemma3.6,
we haveBy substituting (16)
into(15),
we derive the desired formula. D REMARK 3.9. The formula for dimJcuspk,m(0393) proved
in Theorem 3.8 is identicalwith the one
given by Skoruppa
in[10],
derivedby
means of a trace formula(cf.
[11]).
4.
Concluding
remarks1. A
particularly simple
situation is the so-calledgeometric
case, where 0393 =0393(m)
is the full congruencesubgroup of level m
3.Then nj
= m forall j,
andLemma 3.7 shows
Ci
=0, i.e.,
and therefore
2. Because we were
only
able to findexplicit
formulas for thenumbers 03B1j,v
andCi
in thecase nj|m (all j),
it is still an openproblem
to deriveSkoruppa’s
formulafor dim
Jcuspk,m(0393)
of[10]
in the moregeneral case m nj by geometrical methods, using
Theorem 3.4 and Lemma 3.6.3. If we allow
Yr
to haveelliptic
fixedpoints
and cusps of the second kind(still assuming - 1 e F),
we have in addition to take into account thefollowing
newtypes
ofsingular
fibres(cf. [5], §6)
II, II*; III, III*; 7K IV*; I*nj.
Using
thecorresponding
localcoordinates,
which areexplicitly given
in[5], §8,
we
easily
find theappropriate
modifications of Theorems 2.5 and 2.6. The dimensioncomputations
are moredelicate;
one needsanalogues
of Lemma 3.1 andProposition
3.2. We have not touched thisproblem.
If we allow in
addition -1 ~ 0393,
the surfaceXr
will not beelliptic
any more; thefibres of 03C0 become rational curves.
Respecting
thechanged geometrical
nature ofXr,
we are able to find theanalogues
of Theorems 2.5 and 2.6.Again,
thedimension
computations
are more difficult tohandle;
we have done this in thesimple
case r =SL2(Z),
where we rediscover the formula for dimJcuspk,m(0393) given
in
[4].
4. We finish this series of remarks
by mentioning
thefollowing problem:
TheJacobi-Hecke
operators,
introduced in[4],
can beinterpreted
asbeing
inducedby
certaincorrespondences
of theelliptic
surfaceXr
on the space of sectionsH0(X0393,Fk,m). Although
the sheafFk,m
is not anOX0393-module,
we wonder if the trace of the Jacobi-Heckeoperators
can becomputed by
means of theLefschetz-Verdier trace formula
(cf. [12],
p.133).
Acknowledgement
1 would like to thank H.
Knôrrer,
B.Mazur,
G. Stevens and G. Wüstholz forhelpful
discussionsduring
thepreparation
of this note and N.-P.Skoruppa
forsending
me thepreprint [10]. Furthermore,
1 would like to thank the referee forproviding
me with manyimprovements throughout
the whole paper.References
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