A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
A NDREA M ORI
A characterization of integral elliptic automorphic forms
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 21, n
o1 (1994), p. 45-62
<http://www.numdam.org/item?id=ASNSP_1994_4_21_1_45_0>
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of Integral Elliptic Automorphic
FormsANDREA MORI
0. - Introduction
(0.1)
A basicingredient
of the"geometric" approach [1, 6]
to thetheory
of arithmetic modular forms is the so-called
q-expansion principle.
It says,essentially,
that a modularform f
ofweight k
and level N is defined over theZ 2013,~ -al g ebra generated by
its Fouriercoefficients,
gNbeing
aprimitive
n-t
root ofunity.
n-t root of
unity.
The
goal
of this paper is to prove a similarresult,
where instead ofconsidering
the Fourierexpansions,
we considerexpansions
at thepoints corresponding
toelliptic
curves withcomplex multiplications.
Let r be acongruence
subgroup
withoutelliptic
elements ofSL2(Z) acting
on the upperhalf-plane N,
let Yr be the affine canonical model[19]
of thequotient
Xr =
Yr
U{cusps}
its closure andl~r
its field of definition. Our main result is thefollowing:
THEOREM 1
(Integrality Criterion).
Letf be a holomorphic r-automorphic form of weight
k. Let K be anumber field containing
v a non-archimedeanplace of
K such thatXr
hasgood
reduction modulo v, E a CM curvedefined
over K with
ordinary good
reduction modulo vcorresponding
to a K-rationalpoint of
Yr. Let T E M such that C/2
EÐ Z T. Thenf
isdefined
over=
0v n K if
andonly if
and
Pervenuto alla Redazione il 18 Febbraio 1991 e in forma definitiva il 5 Novembre 1993.
for
each r > 0, where8’k
is the r-th iterateof
theMaafi
operatorbk, S2v
is ar / "t:rB
v-adic
period of
E andThe strategy used to prove this result has two distinct
phases. First,
wefind a
significant
localparameter
at a CMpoint x
EYr,
which is toplay
therole of q =
e27riz
in the Fourierexpansion
case.Then,
once this parameter ischosen,
and the formf
isexpanded
around x with respect toit,
the secondproblem
is to compute the coefficients of theexpansion only’ in
terms off
andof the
elliptic
curvecorresponding
to x.The
problem
offinding
agood
localparameter
at a CMpoint
is attacked in Sections 1 and 2. Westudy
the natural action of thecomplex multiplications
on the
ring 6x (the
fiber at x of thejet bundle)
and we show that the local parametereigenvector
of this action is in fact defined over asufficiently large
number field
(Theorem 3). Moreover,
it is shown(with
thespecified
restrictionson the
elliptic
curve under consideration and on theplace
ofreduction)
thatthis
eigenparameter
isstrongly
related to the Serre-Tate parameterclassifying
formal deformations of
ordinary elliptic
curves inpositive
characteristic. This relation with formal geometry allows us to characterize thev-integral jets
at x(Theorem 10).
After a brief review of the different
aspects
of thetheory
of the MaaBoperators (for
a more detailedexposition,
withproofs,
see[3, 4, 8]),
the final part of Section 3 contains anexplicit computation (based mainly
on the results of[9])
of the coefficients. Thiscomputation
will be used to prove Theorem 1 in the last section.(0.2)
In essence, ourproof
of Theorem 1exploits only
the fact that the modularcurves Yr are
naturally
the base ofalgebraic
"universal" families ofelliptic
curves. This seems to
suggest
that our methods can begeneralized
in order toprove
integrality
criteria for much moregeneral automorphic forms;
inparticular,
results of this kind may be of great interest in the case of
compact quotients,
where Fourier
expansions
are not available.In
[15]
the author extends the resultpresented
here to forms of evenweight automorphic
with respect to norm 1subgroups
of an indefinitequaternion
division
algebra over Q (see [19, § 9.2]).
The Shimura curve associated to such analgebra
is the moduli space for thefamily
of abelian surfaces(i.e.
2-dimensional abelian
varieties)
withquatemionic multiplication by
thealgebra
itself
(e.g.
see[12, 18]).
Also,
Theorem 1 can bepartially
extended toprimes dividing
the levelusing
thetheory [10]
of bad reduction of modular curves, see[14].
(0.3)
It should also be noted that apossible important
consequence of the method ofproving
Theorem 1 is that the evaluation of the iterates at roffers a way to attach a v-adic power
series,
i.e. an element of the Iwasawaalgebra,
to apair ( f ,
q : F -GL2(Q)),
wheref
is a v-adic modularform,
F animaginary quadratic
extensionof Q
in which the rationalprime
under vsplits,
and q is an
embedding
normalized in the sense of[19,
Ch.4]. Although
theauthor is
presently
not able to state anyprecise result,
or even aconjecture,
this seems to be relevant for the
theory
ofspecial
values of L-functions.(0.4) Acknowledgements.
This paper is a condensed version of the author’s Ph.D. thesis written at BrandeisUniversity
under thesupervision
of M. Harris.The author wishes to express his
gratitude
to Prof. Harris for the invaluablehelp
andguidance.
An earlier version of this paper and the brief
proof-less presentation [13]
of the main result were written while the author was
supported by
a researchfellowship
of the Istituto Nazionale di Alta Matematica inRome, Italy.
Thereader should be warned that the
expression
for the numbersappearing
in[13, 14]
is correctonly
up to a constant; theright expression
is the one shownhere.
(0.5)
Notations and Conventions. Thesymbols Z, Q
and Cdenote,
asusual,
the
integers,
the rational and thecomplex
numbersrespectively. By
a numberfield
we shallalways
mean a finite extension ofQ,
which will bethought
as asubfield of C
(in
otherwords,
let us fix once for all anembedding a : Q - C).
If v is a non-archimedean
place
of a number field K, thesymbols Kv, 0,
and0t
denote the v-adiccompletion
of K, thering
ofintegers
ofKv,
and thering
of
integers
of the maximal unramified extension ofKv (which
isalso,
for our purposes, the strict henselization ofOv ) respectively.
If X is a scheme over
(the spectrum of)
aring R and
R - R’ is amap of
rings,
we shall denote X00
R’(or simply
X ®R’)
the scheme over R’obtained
by
base extensionalong
the natural mapSpec(R’) - Spec(R).
If a x is a
point
of a scheme X we shall denote(respectively
the stalk at x of the sheaf of the
n-jets (respectively
theoo j ets)
on X.’
If X is a scheme over a DVR R with uniformizer x, and if x :
Spec(R) -
Xis an R-rational
point
of X, set xo =x((0)) and X7r = (7rR).
1. - Local
parameters eigenvectors
ofcomplex multiplications
( 1.1 )
Let K be a number field and x a K-rationalpoint
on the affinemodular curve
Yr
=corresponding
to anelliptic
curve E(endowed
witha
r-structure)
defined over K. Assume that E hascomplex multiplications
andlet
Ko
=Endo(E)
=End(E) 0 Q.
The fieldKo
is aquadratic imaginary
extensionof Q
and we shallalways
assume thatKo
C K. Letbe the natural
quotient
map andpick
r = TE G N such that x. Thecomplex
torus E ® C~ is thusisomorphic to C /A,
whereA, = Z
Theaction of the
complex multiplications
on the torsionpoints
of E 0 C lifts to anembedding qr, : K) - GL(A, o Q). Explicitly,
for any it = a+ ,QT
EK:,
witha,
,Q
CQ,
we haveHence,
acomplex multiplication it
cK,,x
acts on N viaq,(tt), fixing
r. Its actiondoes not induce in
general
an action on the modular curveYr,
because it does not preserve r-orbits. Nevertheless we have:PROPOSITION 2. The action
of
u cK,,’
on Ngives
rise to anautomorphism
PROOF. As
(2)
is a localisomorphism
ofanalytic varieties,
it isenough
to observe
that, by
discreteness of r, we can find openanalytic neighborhoods
U C
M,
T E U, and V cYr,
x E V, such that U -- V viaOr
and:(1)
for each zl , z2 E U, if ZI = iz2 for some i E r then z, = z2;(2)
for each zl, Z2 C U, if = for some -1 E r then z, = z2.Finally,
p, is non-zero(and
in factinvertible)
becauseas
easily computed
from(3).
(1.2)
The rest of this section will be devoted toproving
thefollowing
statement.THEOREM 3. Let K be a number
field
and x a K-rationalpoint
on themodular curve
Yr corresponding
to the CM curve E. Then there is a localparameter U at x, rational over K, which is an
eigenvector for
the actionof
all
complex multiplications of
E on02.
This will be established in three
steps.
First we willcompute explicitly
theaction in terms of the natural
parameter z - T, obtaining
acomplex eigenvector.
Next,
we will establish theK-rationality
of the maps P/1(Proposition 5)
andfinally
we will reduce theproof
of Theorem 3 to anelementary
result of linearalgebra (Lemma 6).
(1.3) Working
with theanalytic
varieties }{ andYr (i.e. working
"overC")
itis natural to choose the local
parameter
Z = z - T to make the identification~ [ [Z] ],
which will be used to make the maps p, ofProposition
2explicit (at
least up to theisomorphism
inducedby (2)).
For alln > 1
and >
= a+ /?7-
E we have’
In
particular
so that defines maps , Ifor For
then we have:
ï r- - - - - I /
PROPOSITION 4. There exists
Un
E which is aA-eigenvector for
all maps with Jj E
K;. A, fter
theprescribed identifications
PROOF. It is
enough
to check that thegiven Un
ismultiplied by
A mod under
(4).
As E does not in factdepend
on it, this will also prove the firstpart
of theproposition.
The result can be proven
by
induction on n, the case n = 1being
obvious.Assume that the result is true for 1 E
6z /m§§
and writeUn
=Vn +,E’-
withYn - Un-,(mod Zn). Then, by
the inductionhypothesis, p,,n(Un)
=aYn
+ cZnand we have to check that c =
Using (4):
This
explicit description
of theeigenvector Un
shows that for n --> oo theUn’s
converge to an element U e02
which is aA-eigenvector
for allcomplex multiplications
of and also a localparameter,
as U Em~ .
From now
on,
we will often think of thering Ox,yr
as the fiber at x ofthe
jet
bundle onYr [2; § IV.16.4.12].
(1.4)
We shall now show that the element U E0~
constructed in theprevious
subsection is in fact rational over K. To do this it is
enough
to establishthe
rationality
over K of at least one of the maps p~ ofProposition
2 withJj E
End(E)
PROPOSITION 5. Let K be a number
field,
and x a K-rationalpoint of Yr corresponding to a
CM curve E withKo
=Endo(E)
C K. Then there is a> E such that the action Pp. on the
fiber of
thejet
bundle at xis rational over K.
PROOF. Let J.t E
End(E),
and let r and E bedefined as in subsection 1.1.
Then,
asexplained
in[19, § 7.2],
defines amodular
correspondence
The action p, can be realized as follows. Look at the maps
where i is the
inclusion,
1rl is theprojection
on the first factor and ~2 is the restriction toY~
of theprojection
on the second factor. Then we have a map of sheaves onYr:
and hence a map of stalks
Now =
EÐ 0,,y,,
the direct sumbeing
extended over the(finite)
set
{z
EY,,1.
Inparticular, O2,yr
is itself a direct summand of theright-hand
side of(5).
Aftercompleting
with respect to therra2-adic topology,
the map p, is
exactly
thecomposition
of(5)
with theprojection
on theO2,Yr
factor.
Thus,
it would beenough
to know that all the varieties and subvarieties under consideration are defined over K. But in factYr
has a model over(a
subfield
of)
K, and the same is true for at least aY~,
with q asspecified, by
[19, §§
7.2 and7.3].
DWe can now show that also the
eigenvectors Un
and U =lim Un
arerational over K. To do
this,
we shallexploit
two facts:(1)
thealgebras 6.,/mn"
have a natural filtration which isrespected by
theaction of the
complex multiplications;
(2)
theeigenvalues
are inKo
C K.Propositions
4 and 5 reduce the task to thefollowing:
LEMMA 6. Let F c L be two
fields.
Let V be afinite
dimensionalvector space over F and
OF
EEnd(V).
Let W = V (8)L F and consider9 L
=OF
(8) 1 EEnd(W). Suppose
that:(1)
V has afiltration
V =V2 D ... D Vn D Vn,l = {O}
with= 1 such that
’ØF(Vi)
CY, for
i =1,...,
n;(2)
For each i =1,..., n
there exists wi EWi = Vi
0 L,wi ~ 0,
such thatfor some ~
E Fl.Then, if ~
is not a rootof unity,
we canfind
vl, ... , Vn E V such thatY’F(vi) = çiVi’
PROOF. We shall construct
inductively, starting
with vn. SinceVn
(8) L =Wn = Lwn,
we can find vnsimply by multiplying
wnby
a suitablescalar.
Suppose
that we havealready
constructed Vk+l, - - - , Vn for somePick v E V such that
~~+1,...~}
is a basis forVk.
Thuswhere a~+1, ... , an c L and a E L . If = an = 0 then v is
already
a~k-eigenvector,
so we may assume that an E Lx(if only
some of thesecoefficients are non-zero, the
following
reductionprocedure
is shorter but not at alldifferent). Apply 1/JL
to both sides of(6)
toget
and subtract
(7)
from(6) multiplied by ~k+1,
The result is whereIterating
thisprocedure
we can eliminate all the coefficients of thevj’s
in(6)
and
finally
write wk = avk for some E V. D Let us fix n > 0 andapply
Lemma 6 to the situationIt is now clear that the
n-jet Un
has a K-rationalmultiple.
The existence of a K-rationalA,-eigenvector
inOx
iseasily
obtainedtaking
the limit. This concludes theproof
of Theorem 3.2. -
Integrality properties
of theeigenparameter
(2.1 )
Let K be asabove,
and let v be aplace
of K with associatedprime
p = p~ C
OK
and residue fieldkv
of characteristic p, such that the canonical modelXr
has a smooth v-adic model.If,
forinstance,
r is one of the groupsr(N), ro(N)
orri(N),
theseplaces v
areexactly
those notdividing
N.Thus,
we will think of
Yr
as a smooth scheme over(the spectrum of) 0t.
Let x be a K-rational
point
ofYr corresponding
to anelliptic
curve Ewith
complex multiplications,
and assume that E hasordinary good
reductionE modulo v. Thus E defines in fact a
Ov r-rational point
ofYr,
which wedenote
by
xagain.
Thegoal
of this section is to characterizenumerically
thefiber in terms of the K-rational
parameter
of Theorem 3. This will be achievedby
Theorem 10.We know from
[2, § IV 16.4.2]
that there are canonicalisomorphisms
1 and
00 = 6xo.
As x is a smoothpoint,
the choice of a0vnr-rational
localparameter
T at x willprovide
a non-canonical identificationFor
any n >
0, the map of sheavesjet (n):
described in[2, § IV.16.3]
defines a map ofrings
For and let be the
composition
of(9)
with the naturalprojection.
Let~r
be the universalelliptic
curve defined over the
ring By extending
the scalars via the map(D n
we can construct
elliptic
curvesE~ = tr
0R~.
This construction isclearly
functorial with
respect
to the natural mapsRm_
1 andR~ 2013~
The
rings R n
are Artinrings
withalgebraically
closed residuefield
k =kv.
In other
words,
the curvesE~
are formal deformations of the curveE®k. By
theSerre-Tate classification of formal deformations of
ordinary
abelian varieties inpositive characteristic,
we can associate to each curveEm
asymmetric (because
of
autoduality)
bilinear formLet us choose
a Z v-generator
P of the Tate module7p(E0k).
Then(10)
definesan element I the elements
converge to
(2.2)
Let uspoint
out that so far the fact that E hascomplex multiplication
hasnot been used. It is a well-known fact that the reduction map
End(E)
~End(E)
is
injective,
and sincet
isordinary, End(t)
can be embeddedin Zp.
Of thetwo
possible
ways to embedEnd(E)
inZp,
the action on the torsionpoints
ofE
corresponds
to that for whichEnd(E)
acts on the Tate module via the latter’snatural Zp-module
structure.Having
chosen thisembedding,
let us denoteby
the
complex multiplication corresponding
to aPROPOSITION 7.
If
E hascomplex multiplications,
the element q - 1of (11) is a formal local
parameter at x,defined
overPROOF. After the identification
(8),
q - 1 - E]
andk[T]/(T2),
so that it isenough
to prove that This is in turnequivalent
toasking
that thep-divisible
groupEo [p°°]
is notisomorphic
to thetrivial extension As the latter is characterized
by
the fact that theshort exact sequence
splits,
theproof
reduces toshowing
that not allendomorphisms
ofE ®
k liftto
endomorphisms
ofEJ[pOO].
Let
[ti]
be acomplex multiplication
such thatfilu
is a unit in0~.
As[ti]
maps
points
of order p topoints
of order p, it isenough
to check that there isno
lifting
of[/z]
toIndeed,
anylifting P,6 :
-~Eo [p]
wouldgive
rise to an
Ró -
linear mapA(P)6
-A(P)6
of thecorresponding Hopf algebra.
This map would have to be the
identity
onRo
= k EÐ(m~/m2) ® k,
which isimpossible
because the action of the chosen on(mx/m 2) (&
k is not trivial.COROLLARY 8. There is a
(non-canonical) isomorphism
PROOF. It is the identification
(8).
See also[16,
Remarks(2.3)
Now weexplain
how thecomplex multiplications
act on theparameter q-1.
Since for CM curves the Rosati involution
corresponds
tocomplex conjugation, End(E)
acts onTp(k 0 k)
xTp(E ® k)
as(Pi , P2) = (API, jlP2).
We haveproved
in theprevious
subsection that thecomplex multiplications
do not liftto the deformations
E~.
This will be still true for ageneral
formal deformationE/R (R
an Artin localring
with residue fieldk),
because therequirement
dueto the Serre-Tate classification theorem is not met. Indeed
for
generic E, [~u].
Nevertheless thefollowing
result holds:LEMMA 9. Let E be a
deformation of .9 0
k over an Artinring
R withresidue
field k,
and acomplex multiplication of
E.If
J.t then there exists adeformation E~
over R and a map E ----+E~ lifting
PROOF. Let be the bilinear form associated to E. De-
fine Clearly, q,(-, -)
isa,
bilinear form onbe the deformation of
E ®
k over R suchr I
thatq
. Then and theexistence of the
lifting
isguaranteed again by
the theorem of Serre and Tate.0 This discussion shows that the action of the
complex multiplications,
corresponding
to it sits in the action ofZ ’
onk)
xTp(E 0 k), Gm(R)) given by z ~ ~ _
The latter action is functorial withrespect
to the natural mapsR£ - R~
1 andR,’ ,- 1. By taking
thelimit,
it is therefore clear that also the
parameter
q E 1 + mz is transformedby
thecomplex multiplications according
to the law q -+qfl/ J1.
(2.4)
We can now prove thefollowing
result.THEOREM 10. Let K be a number
field,
p c K aprime
as in(2.1)
and x a
Kp-rational point of
the modular curveYr corresponding
to a CMcurve E with
ordinary good
reduction modulo p. Then there is aKp-rational
local parameter T at x which is an
eigenvector for
the actionof
thecomplex multiplications of
E on thefiber
at xof
thejet
bundle onYr.
Moreover, an00
element
E an i
Tn EKp[[T]]
isp-integral if
andonly if
anE Op
andn=O n!
where the
coefficients
aredefined by
theformal identity
PROOF. Consider
By
the resultsobtained in the
previous subsection, Q
is aAu,-eigenvector
for the action of thecomplex multiplications.
Therefore U =0152Q,
where U is the localparameter
atx constructed in Section
1,
and a E0152 fO. Up
tomultiplying
Uby
a scalarin
K§
we mayalways
assume that a is a unit in Let T be anyparameter
defined overKv satisfying
a relationwith a a unit in Then is defined over
0/,
seeBut also o so that
eT -
1 is defined overFinally,
the second part of the statement is provenexactly
as in[5,
Theo-rem
13].
D3. -
Computing
the coefficients via the MaaBoperators (3 .1 )
MaaB[11]
introduced the differentialoperators
(and
theanalogous
for theSiegel
upperhalf-space).
Write andlet k be a
positive integer.
Define theoperator
For any
subgroup
r of finite index inSL2(Z),
letGrcr)
denote the space of C°°-modular forms ofweight
k withrespect
to r.Then,
it isroutinely
checked that the
operators 6k
descend tooperators 6k : Gr(r)
--;The MaaB
operators (14)
aresubject
to differentinterpretations
asautomorphic
forms are seen from different
points
ofview,
asbriefly explained
in the nexttwo subsections.
(3.2)
A(possibly C°°)
modular formf
ofweight k
withrespect
to asubgroup
rof finite index in the full modular group
SL2(Z)
can be lifted to a C°° functionon G =
SL2(R),
definedby
the formulaThe
automorphic
relation satisfiedby f
forces upon the relationswhere is the maximal
compact subgroup
of G that
stabilizes
i E N.Conversely,
if0 is
a C°°-function on Gsatisfying
the relations
(15),
then we can define ar-automorphic
form ofweight k
by
I - -1 ,An element I A E
Lie(G)
acts on the C°°-functions on Gby
’he
adjoint
action of K induces adecomposition
with
and
If
f
is ar-automorphic
form ofweight
k, the formulae(16) imply
that thefunction satisfies the relations
(15)
with k + 2 in theplace
of k.Hence,
we can define an
operator Dk :
. Anexplicit computation,
see[4],
shows that(3.3)
Consider now theanalytic family
ofelliptic
curves 03C0 :Ey
-->JI,
whose fiber over T E JI is thecomplex
torusC /Z
and thealgebraic
familiesx :
Er
-Yr
obtained as the space of the orbits of the action of r onEV.
Toeach of these
families,
we can attach the relative de Rhamcohomology
bundleHDR,
whose fiber at T c N(or x
EYr)
isjust
the first de Rham group of thecorresponding elliptic
curve.Furthermore,
we will denoteH~
the associated C°°-bundles. Thefiber-by-fiber Hodge decomposition
induces asplitting
with an
isomorphism
of C°°-bundles Letbe the
projection
definedby (17)
and theisomorphism just
mentioned. If k is apositive integer,
we can now define a Coo differential operator8k : Wok through
thefollowing
steps(where S21
denotes the bundle of 1-forms on thebase):
Step
1: EmbedStep
2:Apply
the map obtainedby product
rulefrom the
Gauj3-Manin
connectionStep
3:Compose
.L theresult
with theKodaira-Spencer isomorphism
to land in i
Step
4: Use the obviousprojection
inducedby (18) Sk(Split) :
to send the result to
It is shown in
[4] that,
after the identificationf H f(2xi du) ok
betweenelements of
G~ (r)
andglobal
sections ofWok,
the operatorsok
coincide with theoperators Dk
defined in theprevious
subsection.(3.4) Suppose
that E is anelliptic
curve withcomplex multiplications,
definedover a number field K.
Any complex multiplication >
acts on the groupHDR(E/K) inducing
aneigenspace decomposition
whichis in fact
independent
of 1L.Furthermore,
thedecomposition
ofHDR(E, C)
=1 R(EIK) o C
inducedby
it coincides with theHodge decomposition, [7,
Lemma
4.0.7].
This is an essentialingredient
for a number of results about thealgebraicity
of the values that modular forms attain at CMpoints.
Inparticular,
it shows that at a
point
y EYr corresponding
to E, theoperator
will be
actually
defined on the fibers of thealgebraic
bundles.Let R be a
sufficiently large ring
over which E is defined and such that the R-moduleQ1/R
is free. The choice of asingle
R-rational invariant 1-formw on E induces an identification of with a copy of R; thus
(19)
definesisomorphisms w®x
---~ R,and, considering
the r-th iterate of8k, isomorphisms
-, R. Katz proves in[8]
thefollowing
result
(where,
in view of ourapplication,
the restrictions on R areautomatically
satisfied as E has
ordinary good reduction):
THEOREM 11. Let E be a CM curve
defined
over asubring
R w aR-rational invariant
7-/i9A7M
on E, andf a modular form of weight
kdefined
over R. Then:
where
f is identified
to a sectionof ~~yok
and y is thepoint corresponding
toE ~C
(3.5)
One of theadvantages
of thealgebraic theory
of the MaaBoperators
as described in subsection 3.3 is that it is well suited for
generalizations.
Inparticular,
the entiretheory
can be carried over to thep-adic
case, when oneuses, instead of
(17),
the unit root spacedecomposition
of thep-adic
de Rhambundle
provided by
the Frobenius map.It turns out that for CM curves with
ordinary good reduction,
also the unit root spacedecomposition
coincides with theHodge decomposition, [7,
Lemma8.0.13]). Therefore, regarding
a modular form defined over ap-adic ring
R as ap-adic
modular form(in
the sense of[8, §§ 1.9-10]),
the values at a CM curvewith
ordinary good
reduction of and itsp-adic counterpart
coincide. We willexploit
this fact in the next subsection.(3.6)
Let us go back to the situation and notation of Section 2. Consider the universal formal deformation £ ofE 0
k. Theelliptic
curve 6 is defined overthe
ring R,
analgebra
over the Witt vectorsW(k).
Since theelliptic
curvesE~
are deformations of
E ® k
to Artinrings,
for each of them there is a"classifying map" on 2013~ R~
such thatEm
=E~1/J~ 4. Passing
to the limit over mand n, we can construct a map
’~~
and,
inparticular,
anelliptic
curveEjet
defined over thering
ofpv-integral jets, by
Let
f
be aholomorphic r-automorphic
form ofweight
k defined over(a subring of)
C. It is understood that we may extend the scalars where theelliptic
curves under consideration aredefined,
in order to be able to evaluatef
at them.Let us recall that the construction of the parameter q - 1 involved
choosing
a
Z p-generator
P of the Tate moduleUsing
onceagain
theself-duality
of
E,
Pdetermines,
as in[9, § 3.3],
a non-zero invariant 1-formw(P)
on e.This form allows us to
identify
the fiber of w(as
well as itspowers)
overthe R-rational
point corresponding to e,
with R itself. Thus we can writef (~) = f ® w(P)®k
where1 E
2 andf(Ejet) = (jet f )(x) _ ~( f )
(&(O*W(p)),,k.
Set/jet
=Jt
and wjet = Let us now use the parameterQ
=log
q toidentify fjet
with a powerseries,
i. e. writeObserve that the coefficients
bn(f) depend
in fact also on P. If P’ = vP withv is another Z
p-generator
ofTp(E 0 k),
thenas
easily
seen.We shall now use the identification
(20)
to compute the value at x of for r =1,2,....
We aregoing
to follow the "instructions" outlined in subsection3.3,
and we will makefrequent
use of the results and notations of[9].
Infact,
we will compute the value at x of the transformed off by
thep-adic
MaaBoperators.
As remarked in theprevious subsection,
this will notchange
the final result.Step
l:Computing
theGauj3-Manin
connection.Let P* be the dual generator of
k),Zp)
c and letFix(P*)
be thelifting
of P* to the unit rootsubspace. Then, by [9,
Theorem4.3.1], V(w(P))
=dQ,
andV(Fix(P*))
= 0.Therefore,
we haveStep
2:Composing
with theKodaira-Spencer
map.We need to
compute
theimage
of the differentialdQ
under theKodaira-Spencer
map KS : SZ -~
w 02.
In[9]
Katz constructs theKodaira-Spencer
map as a map Kod : _w --~ Lie ® Q and proves that under the canonicalpairing w
o Lie -~ Rone has
w(P). Kod(w(P))
=dQ. Therefore,
we must haveKS(dQ)
=w(p)102 ,
andfrom the
computation
made in step 1:Step
3:Projection.
Applying
thep-adic splitting
inducedby
the unit root spacedecomposition,
theterm in
(22) containing Fix(P*)
vanishes and weget
The
original
curve can be recovered fromEjet just setting formally Q
= 0 once theisomorphism 0t[[q - 1]]
is fixed. Therefore from the identification(20)
and formula(23)
we obtainwhose
right
hand side isreally independent
on P(as
it mustbe)
aseasily
confirmed
by
the relations(21).
It is also clear that thecomputation
canbe iterated. Since the unit root
subspace
is horizontal for the GauB-Maninconnection,
we have4. - Proof of the main result
(4.1)
We shall now define theperiod S2v
of Eentering
in the definition of the numbers Since E hascomplex multiplications,
we may assume that E has a smooth modelEv
over for each non-archimedeanplace
of K. The0v>-module H°(E, Q1/0,,)
ofv-integral
invariant 1-forms on E is free. Let wv be agenerator. By definition,
wv is defined up to a v- adic unit. Pick T E )Isuch that there is an
isomorphism (D : C/Z
Then theglobal
differential 1-form will be a scalar
multiple
of the 1-form definedby
dz, i.e. we maywrite, by
abuse ofnotation,
= for someS2v
E C. ThisI
complex
number can be seen as aperiod
ofo
The choice of a different T to write an
isomorphism
ofcomplex
tori asabove,
is reflected in a different normalization of the
period
lattice ofE,
which alters the numberby
aglobal
unit inOK. Combining
the effects of the differentchoices, SZv
remains defined up to av-adic
unit.Let us remark that if K has class number 1, the choice of a v-adic
period
for E can be
globalized. Indeed,
in that case the moduleHO(E,
is free:any
generator
wo may serve as wv for all v’s at the same time.(4.2)
We can now use thecomputation
made in subsection 3.6 to prove ourintegrality
criterion(Theorem 1).
To avoid anyambiguity,
we shall denoteby /alg
thealgebraic
modular form defined over C, obtained fromf
via the relation Let us start withf (i.e. falg)
defined over =OvnK.
From the discussionpreceding
Theorem 11 we know that also the form must bev-integral.
Now
compute:
Thus,
Let i be such that
w;et(x)
=Comparing
the abovecomputation
of with
(24)
and(20) yields
As the