N A L E S E D L ’IN IT ST T U
F O U R IE
ANNALES
DE
L’INSTITUT FOURIER
Fabrizio ANDREATTA
The small Schottky-Jung locus in positive characteristics different from two Tome 53, no1 (2003), p. 69-106.
<http://aif.cedram.org/item?id=AIF_2003__53_1_69_0>
© Association des Annales de l’institut Fourier, 2003, tous droits réservés.
L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). Toute re- production en tout ou partie cet article sous quelque forme que ce soit pour tout usage autre que l’utilisation à fin strictement per- sonnelle du copiste est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.
cedram
Article mis en ligne dans le cadre du
Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/
THE SMALL SCHOTTKY-JUNG LOCUS IN POSITIVE
CHARACTERISTICS DIFFERENT FROM TWO
by
Fabrizio ANDREATTA1. Introduction.
In this paper we
investigate
theproblem
ofcharacterizing
the idealsheaf
defining
the locus of Jacobians of curves of genus g in the moduli space ofprincipally polarized
abelian varieties ofdimension g
over any field of characteristic different from 2. We use the so-calledSchottky- Jung
relations. In[vG],
Thm1.6,
it is proven that over C the irreduciblecomponent
of the locus definedby
theSchottky-Jung
relationscontaining
the Jacobians consists
only
of Jacobians. See also[Dol]
and[Do2],
Ch. 2.The idea of B. van Geemen is to reduce the
problem
to thestudy
of theSchottky-Jung
relations induced to theboundary
of the moduli space ofprincipally polarized
abelian varieties and toapply
an inductionprocedure.
We borrow and
generalize
this idea to prove thefollowing
theorem.Let g
be an
integer >
2. Let I~ be a field of characteristic different from 2. LetAg
be the moduli space of
principally polarized
abelian varieties of dimension g. LetMg
be the moduli space of smooth curves of genus g. Let be the closed subscheme of ® l~ defined as the scheme theoreticimage
ofTig
® I~ via the Torelli map. This is the map which associates to a curveits Jacobian. Let be the closed subscheme of ® 1~ defined
by
theSchottky-Jung
relations overk ;
see 4.6.THEOREM. The
irreducible component
ofcontaining
is
equal
to3g,k-
’
Keywords: Schottky-Jung relations - Theta functions - Mumford’s uniformization.
Math. classification: 14H42.
The first
novelty
of ourapproach
is that we workpurely algebraically.
In
§2
we review thePrym
construction fordegenerating
curves. In§3
we
briefly
recall the formalism of Mumford’s theta functions. These are a valuable substitute for the classical theta functions when one does not work over C. The maindifficulty
is to deduce theSchottky-Jung
relationsbetween suitable Mumford’s theta functions from the
Prym
construction.We overcome the
difficulty
in§4 following closely
an idea of Mumford’s sketched in[Mu2].
The secondnovelty
is the use in our context of therecent progress on toroidal
compactifications
of moduli spaces ofpolarized
abelian varieties. We refer the reader to
[FC]
for the construction of suchcompactifications.
In[FC]
adescription
ofdegenerating
semiabelian schemes over affineschemes, satisfying
suitableconditions,
isgiven
interms of so-called
"degeneration
data". It is also proven that the families described in this way cover theboundary
of toroidalcompactifications
ofmoduli spaces of
polarized
abelian varieties(possibly
with extrastructure).
The Fourier-Jacobi
expansion
of thetafunctions,
as reviewed in§5,
canbe described in terms of
degeneration
data.Conversely,
thedegeneration
data are encoded in the Fourier-Jacobi
expansion
of theta functions. This allows us to translate theSchottky-Jung relations,
induced to theboundary,
into restrictions on the
degeneration
data of semiabelian schemessatisfying
these relations. The Fourier-Jacobi
expansion
enables us also to godeeper
in the
boundary
than in[vG],
whereonly
rank 1degenerations
are used.The
advantage
is that we can focus onneighborhoods
ofpoints
of theboundary
whose abelianpart
is of lowdimension,
in our caseequal
to2,
and which
consequently
are easy to handle. This is the mainingredient
inthe
proof
of the extension of Van Geemen’s theorem contained in§7.
Contents.
1. Introduction.
2. The Prym variety.
3. Mumford’s theta functions.
4. The Schottky-Jung relations.
5. Fourier-Jacobi expansion of the Schottky-Jung relations.
6. The heat equation.
7. Van Geemen’s theorem.
Bibliography.
2. The
Prym variety.
In this section we review the
Prym
construction. This appears in[Mu4]
for covers of smooth curves(over
afield)
and in[Be]
for ad-missible covers of semistable curves
(over
afield).
We extend it to the caseof families of semistable curves over an
integral
normal base scheme with smoothgeneric
fibers. This appearspartly
in[Be], §6.2,
withemphasis
on the
Prym variety
itself. Since we are interested in theprecise
relationbetween the
Prym variety
and the Jacobian varieties it arisesfrom,
wegive
some details. ’
2.1. The
setup.
Let S’ be an
integral
normal scheme with function field K. Assume that 2 is invertible in S. Letbe a semistable curve over ,S
i.e.,
a proper and flatmorphism
whosegeometric
fibers arereduced, connected,
of dimension 1 and haveonly ordinary
doublepoints
assingularities. Suppose
that1 ) f is
smooth overK;
2)
C has genus2g - 1
for somepositive integer
g;3)
there exists anautomorphism t
ofC’,lover
,S’ such that3.a) t
has order2;
3.b) t
actsfreely
on the smoothpart
Csm off ;
3.c)
forany geometric point s
of S and anyordinary
doublepoint
c E
Cs
fixedby
t, the branches ofCs
at c are notinterchanged by
¿ s .Consider the
quotient
mapDenote
by
the induced
morphism. Then,
1) by [Be],
Lemma3.1, f
defines a semistable curve overS;
2)
themorphism
7r restricted toCsm
is finite and etale. Inparticular, f
is smooth over
K;
3) by
the Hurwitz formula C has genus g.Let ,S’° be the open subscheme of
S,
wheref :
C - S is smooth.2.2. Remark. - The
morphism
7r is an admissiblecovering
in thesense of
[HM],
p. 57. This notion appearsalready
in[Be],
p. 157. Itsimportance
is due to the fact that suchcoverings
arise in the process ofcompactifying
the moduli space ofetale,
2 : 1coverings
of smooth curvesof genus g. See
[Be],
pp.180,
Part(b)
and[HM], §4,
Theorem 4.2.3. The associated Picard varieties.
Consider the
fppf
sheavesThey
are definedby
thepresheaves associating
to anfppf
cover T - Sthe abelian group of line bundles on C x s T
(resp.
onC
x sT),
which arefiberwise over T of
multidegree 0,
modulo the line bundlescoming
from Tby pull-back. By [BLR],
Theorem9.4.1, they
arerepresented by
semiabelian schemes over Si.e., by smooth, separated,
commutative group schemes overS such that the fiber over any
geometric point
of S is the extension of anabelian
variety by
a torus. Note that over the open subscheme S° of S wheref
is smooth the semiabelian schemesare abelian and are endowed with
principal polarizations;
see[BLR], Prop.
9.4.4.Finally,
letbe the
morphism
inducedby
7rby functoriality
ofPic° .
2.4. The theta torsors.
After
possibly replacing
,S’ with an etalesurjective
cover, choose aneffective Cartier divisor r, on C x s S° relative to S° whose square is
isomorphic
to thedualizing
sheaf on C x s S°. Note that 7r*(K)
is aneffective
Cartier divisor. Its square is
isomorphic
to thedualizing
sheaf onC
x sSO;
cf.
[Be],
Lemma 3.2. Define the theta divisoron x x s S’°
(resp. on y
x sby translating
theimage
ofthe g -
lthsymmetric
power of C inPicg-1(C
x s to xPic° (C
x sS° /S°) (resp.
theimage
of the2g -
2thsymmetric
powerof
C
X s So in : via translationby
-~(resp. by -7r*(K)).
The Riemann-Roch theoremimplies
that the divisors and are
symmetric. Moreover, they
inducethe
given principal polarizations
on x x s S°and y
x s S°. Denoteby
the associated
symmetric
which werigidify along
theidentity
element
(resp. By [Br], Prop. 2.4,
ituniquely
definesa cubical over x
x s S° (resp. Y By [MB], Theorem
11.3.3and
[MB],
Theorem11.1.1,
there exists aunique
cubical£x
(resp.
on x(resp.
ony) extending (resp.
2.5. Remark. - The line bundles on a smooth curve whose square
are
isomorphic
to thedualizing
sheaf are called theta characteristics.Hence,
the chosen in the
previous
section is a theta characteristic.By
Riemann’ssingularity theorem,
h(C x s S°, K)
is alocally
free sheaf of rankequal
to themultiplicity
of the divisor theidentity.
We choose K so that therank of
r (K,
C x s is even is a so-called even theta characteristic.2.6. Remark. - The discussion in 2.4
depends
on the choice of the theta characteristic r~. The definition is needed toget
theSchottky-Jung
relations. In
general,
thedualizing
sheaf of C - ,S’ does not admit a theta characteristic. Forexample,
this is the caseif,
for somegeometric point
s E
S,
thepull-back
of thedualizing
sheaf ofCs
to the normalization ofsome irreducible
component
ofCs
has odddegree.
Thisexplains why
weworked over the open subscheme S° . On
the
other hand:2.7. PROPOSITION. -
Étale locally
on S one may choose a line bundleL (resp. L)
overC (resp. C)
such that the locusdefines an effective Cartier divisor in
Y (resp. X)
relative to S. Over S° it coincides with a translation of(resp.
Proof. This is the main result of
[Be], §2. See,
inparticular, [Be],
Remark 2.4.
2.8. Remark. - For the reader not familiar with the
concept
of cubicaltorsors,
wesimply
remark thatthey
are ageneralization
of theconcept
ofpolarization
in the context of abelian varieties to thecategory
of semiabelian schemes. See[FC],
Remark 1.2.4 for aquick
introduction and[Br], Chap.
I-III or[MB], Chap.
I for a fullexposition
of the notion of cubical(Gm-torsors.
2.9. Duals and
polarizations.
By [FC], §II.2,
there exist a semiabelian schemext
over ,S’ and abiextension
extending
the abelian schemeXK,
dual toxK,
and the Poincare biextensionover
XK Analogous
definitions aregiven
forY
instead of x. Denoteby
the
isomorphisms extending
theprincipal polarizations
defined over K.By [FC], Prop. 1.2.7,
there exists aunique homomorphism
extending
the dual of 2.10. The norm map.Let T be a scheme over S. Let L be a line bundle on
C x S T,
fiberwiseover T of
multidegree
0. Letbe the
isomorphism
inducedby flipping
the two factors. DefineBy
descenttheory
it is a line bundle on the open sublocus of C x s T where7r x s T is etale. A local
computation
around thepoints
where 7r is not etaleshows that
Nm(L)
is a line bundle.2.11. PROPOSITION. - The Norm map
Nm: y
---* X1 )
is a grouphomomorphism;
2)
satisfies3)
satisfies4)
is smooth.Proof. Claim
(1)
is clear.By [Mu4],
p.328, (i)
theequality
claimedin
(2)
holds overK. Hence,
Claim(2)
holds. Claim(3)
follows from a directcomputation. By (3)
we deduce that Nm issurjective
both on the levels of varieties andtangent
spaces.Hence,
it is smooth.2.12. The kernel
Let s E S be a
geometric point.
Denoteby
asubscript s
the basechange
from S’ to s.Let q
EKer(7r;). Suppose
that q7~
0.Then,
q is the class of a line bundle L onCs.
SinceNms o7r§ = [2],
we have thatL~ ~ Ocs .
Choose such an
isomorphism
a. It defines the structure of aOcs-algebra
on the coherent
Ocs-module Dcs
0L;
see[Mu4],
p. 326. The associated schemeis finite and etale of
degree
2. Theisomorphism
cx definescanonically
anisomorphism ,~: ~* (L) ~ OD. Moreover,
for any scheme T over s, anymorphism 1b :
T -Cs
and anyisomorphism
’1:1b* (L) E# OT,
there is aunique morphism
v: T - D ofC,-schemes
such that = -y. Inparticular,
weget
amorphism
ofCs-schemes
which must be an
isomorphism.
Vice versa, suppose that
7rs:Cs
-C,
is étale.Then, 7rs,*(O¿)
isa coherent
Oc,,-algebra, locally
free of rank 2 asOcs-module.
The map2-1 Tracer ,
defines asplitting
as
Oc,, -modules.
Thealgebra
structureimplies
thatL2 is
trivial. SinceCS
is
connected,
L itself is not trivial. We conclude:2.13. PROPOSITION. - Let
Then,
H is aquasi-finite
and flat group scheme over S. If s E S is ageometric point,
we have L1) Hs
=101
if andonly if 1rs is
notetale;
2)
over the open subscheme S’ of S where 7r is6tale, Z/2Z.
Wedenote
byq
thegenerator.
2.14. The
Prym variety.
Define
as the inverse
image
viaAy
of theidentity component
of This is called thePrym variety
associated to thecovering
7r.Since
Nm,
andconsequently 7r*,t,
is a smoothmorphism,
the scheme P is asemiabelian scheme of relative
dimension g -
1 over S.Compare
with[Be],
§6.2.
For any line bundle L on
C,
ofmultidegree
0 fiberwise overS,
the linebundle L2 = (L ® ~* (L)) ® (L ® ~* (L-1 ))
is in theimage
of X x sKer (7r*> ) .
Indeed,
L® ~* (L) _ 7r* (Nm(L))
andNm (L
0¿*(L-1))
is trivial.Hence,
the
morphism
is
surjective
fiberwise over ,5’and,
inparticular,
it is anisogeny.
The
following proposition
extends to thepresent
case the well- known factsconcerning
thePrym
construction for smooth curves over analgebraically
closed field contained in[Mu4].
2.15. PROPOSITION. - The
following
hold:1. iwe have an
eq uali ty
of effective Cartier divisorswhere is a
symmetric
divisor on P relative to ,S’°inducing
aprincipal polarization
on 7~ xS,S’°.
Inparticular,
there is asymmetric
cubicalGm -torsor L-p
over P such thatas
symmetric
cubicalGm-torsors
over P.2. We have an
equality
of effective Cartier divisorsHere, try
denotes the translationby
q on X x s So. Inparticular, (7r*) * (£y)
is
isomorphic
to assymmetric
cubical3. We have a cartesian
diagram
where is the
symmetric
cubicalgot by descending C2 x
to ..
4. Let
HK
be theorthogonal
ofHK
insideX[2]K
withrespect
to the Weilpairing.
Thepull back
toHK /HK
of the cubical torsor descended onXKIHK
from is trivial. Inparticular,
it induces asymplectic
structureon
HK /HK .
There is anisomorphism
preserving
thesymplectic structures,
such that the kernel x xyx
is thegraph of 0.
Proof. - To prove the statements in
(1)
and(2) concerning
thedivisors,
we may assume that S’ =Spec(K)
and K isalgebraically
closed.See
[Mu4], Prop.
p. 342 for( 1 ) .
See[Mu4], Corollary
5.3 for(2).
For theproof
of(3)
and(4)
overK,
see thearguments
of[Mu4],
p. 330. Let G bea semiabelian scheme over S. Since ,S’ is
normal,
thecategory
ofsymmetric
cubical
Gm-torsors
over G isequivalent
to thecategory
ofsymmetric
cubicalGm-torsors
overGK [Br], Prop.
2.4.By
theequivalence
ofcategories just stated,
statements(1), (2),
and(3)
follow sincethey
hold over K.2.16. Remark. - For a more
geometric
andexplicit approach
in thecase of Mumford’s curves see
[vS].
3.
Mumford’s theta functions.
In this section we
briefly
review Mumford’s construction of 2-adic theta functions as in[Mul].
Since we are interested indegenerations
oftheta functions on
S,
weslightly generalize
theapproach
of Mumford.3.1. SOME NOTATIONS. - Let A be a semiabelian scheme over
S,
abelian over K. be a
symmetric Gm-torsor
over A. Fix arigidification
x A 0 --~
A1
of the associated line bundle L.By [Br], Prop.
2.4 we canconsider ,C as a cubical
Gm -torsor
over A.3.2. DEFINITION. - Let
K(,C)
be the Zariski closure in A of the kernel of thepolarization AK - AK
inducedby £K. By ~MB~,
Theo-rem
IV.2.4,
it is a group schemequasi-finite
and flat over S.3.3. DEFINITION. - Let n be an
integer.
Define(An,Pn)
as thecouple consisting
ofAn =
A and themorphism
The is an inverse
system
via the naturalmorphisms
defined.,
for allintegers
m and n such that m - n, asmultiplication by
2n-,.
Compare
with[Mu1J,
Definition 7.1.For any
integer
n define thefppf
sheafAn [2°°]
as the direct limitwhere
An [2’]
is the kernel ofmultiplication by
2m.Define the 2-divisible
fppf
sheafV(A)
as theprojective
limit overn eZ:
where the transition
morphisms
are induced from themorphisms
pn,,,,. For anyinteger n
defines theprojection morphism
Define the lattice
T(A)
insideV(A) by
It acts
by
translation onV(A). Compare
with[Mull,
Definition 7.2.Finally,
definer(L)
as the direct limit over n E N:The transition
morphisms
are definedby
thepullbacks
of sections via themorphisms Compare
with[Mull,
Definition 7.3 and[Mull, §7,
pp. 108-109.
3.4. Remark. - We
prefer
to deal withV(A)
as anfppf
sheaf sincewe are interested in
degenerations
of thetafunctions,
while Mumford worksover
algebraically
closed fields in order to be able to find a basis of theQ2- topological
vector space3.5. DEFINITION
([Mul],
Definition7.4).
- Define the elements of the infinite theta group~(,C)
as thepairs
of elements(x,
where0 x is an element
of V (A);
o let nx be the smallest
integer
n for whichbelongs
to thegroup
I~ (pn (,C)) ;
see 3.6. The settOn In,
with ninteger
such that n > nx, is acompatible system
ofautomorphisms
oflifting
translationby
p (x)
-n onAn.
There is a natural action
Moreover, g(L)
sits in an exact sequencesuch that the torus
Gm,s
is in the center ofg(L).
Inparticular,
weget
a skewsymmetric pairing
as follows. If X, Y E
V (A)
andx, y
Eg(L)
areliftings
of x, y, thenSee
§ 7,
pp. 103-104.Let v be a
non-negative integer.
Denoteby ~ (pv (,C) )
the finite theta group onAv
defined as in[MB],
TheoremIV.2.4(iii).
Thefollowing
hold:o its fiber over K is the theta group of the line bundle associated
[MB],
TheoremIV.2.4(ii).
~ it acts on
~ it sits in an exact sequence:
[MB],
TheoremIv.2.4(iii);
~
by
construction there is a naturalsurjective homomorphism
of group schemes
compatible
with the induced action on~ the
morphism
is an
isomorphism.
The limit on the RHS is taken over thenon-negative
integers
n.Define
The group is the
subgroup
of elements of~(,C) acting trivially
onL(Av,pv*(L))
3.6. Remark
( ~Mul~ ,
"4 > 2"Lemma,
Section7).
- If s is apositive integer [s]*(£)
isisomorphic
to£s2
andA~s2~
is contained inK(,CS2 ) . Hence,
the
integer
nx of 3.5 exists.3.7 DEFINITION
( ~Mul~ ,
Definition7.5).
- The exact sequence defined in 3.5 for~(,C)
admits a naturalright splitting
cr as sets defined asfollows:
Let a = be an element
of V(A).
Let no be aninteger
suchthat for any n > no we have an -
2bn with bn
an element inK (pn (,C)) .
For
any n >
no choose cn =above bn
such that1 ~n 1
where’Øn
is anyisomorphism of p§ (£) lifting ~-1~
on
An.
DefineIt is an element
of 9(,C)
above a.3.8. Remark
([Mul],
Lemma7.3).
- If x and y are two elements of then3.9. DEFINITION
([Mul], §8,
p.113).
- Define the thetamorphism
as follows:
If Q is
an elementof T (L)
and a =(an)nEZ is
an element let~,~(a) _ ~Po((~(-a)(~))(~))~
>where the action
of a((-a)
is definedby
the action ofg(L)
onr(L) (3.5),
the map cpo is defined in 3.l.
In
particular,
suppose that a, x EV(A). By
3.8Compare
withProperty
8.L3.10. DEFINITION
([Mul], §2,
p.304).
- We define aquadratic
character -
as follows. Let
0:
L ~[- 11 * (L)
be anisomorphism
normalized so thatL(O)
-[- 1] * (L) (0) - L(O)
is theidentity;
it exists since L issymmetric.
Defineby L(x) ~ L(-x) = L(x) being multiplication by
Note thatPO
identifies..
By [Mull,
Lemma 7.4 the charactereL
satisfies thefollowing:
if x EJ(o and y
ET(A)
is itsimage
inV (A),
thenBy
the discussionof [Mull, § 7,
p.108, given
thepolarization
on A definedby .C,
the structure as abstract group and the section a:V(A)
-g(£:.),
there is a 1-1
correspondence
between1.
quadratic
characters2. line bundles on A
defining
thegiven polarization.
3.11. PROPOSITION. - Let g: B --+ A be a
morphism
of semiabelian schemes. Let 1: and M ~g*(£)
besymmetric,
cubicalGm-torsors
withcompatible rigidifications.
Let/3A
be an elementof r(L)
and let a =(an)
be an element
of V(B). Then,
Moreover,
for any a and b in
V(B) and, finally,
for any a
3.12. ASSUMPTION.
Suppose
from now until the end of the section that the base ,S’ is local with maximal ideal I andalgebraically
closed residue field.
Suppose
that A is an abelian scheme over S. Choose acompatible system
of 2nth roots ofunity (~2n)
inOs
for allnon-negative integers
n.Suppose
that L hasdegree
1. be aglobal
section(unique
up to
constant)
of theassociated line
bundle L. WritegA := GBA
We can
apply
Mumford’stheory
of theta functions as in[Mul].
Mumfordworks over an
algebraically
closed field. With ourassumptions
we canextend his
theory
to our context.3.13. DEFINITION. -
Let g
be the dimension of A. Define the bilinearpairing
as follows. Let
(a, b) :== alb1
+... +agbg
and let V2 be the 2-adic valuation.Put -y
and aequal
to 0if v2 ( (a, b~ ~ >
0 andotherwise. Consider
Qg
xQg
as a constantQ2-vector
spacesheaf
over Swith the
symplectic
structure definedby
Define
The
symplectic
structure onQ~
xQ~
defines a group structureon gg
andan exact sequence:
cf.
§ 7,
p. 106.Define a full theta structure on
(A, L)
to be anisomorphism
assheaves
ofQ2-vector
spaces over S:such that cA
respects
thesymplectic
structures and sendsT(A)
toZ~
xZ~.
By
3.12 suchisomorphisms
exist. Fix one.The
isomorphism
cA defines anisomorphism
of groupssee
[Mul],
Definition 7.8 and the discussion after that. Theisomorphism
cA is theunique
onecompatible
with cA andsatisfying
thefollowing.
Let a bein
V(A)
and letcA (a) _ (x, l ) .
ThenAs in
[Mull,
Lemma7.4,
it follows that for all a ET(A), putting
The
group 9g (and, hence, g(L)
viacA)
acts onHg
as follows:Recall that
1tg
is theunique
admissible irreduciblerepresentation
ofweight 1 of 9. (
and hence up toisomorphism.
See[Mull,
Definition 7.9 and the theorem after it.The
description
of therepresentation theory
of the isgiven
in pp.114-115, by
thefollowing diagram:
where
r (L)
is defined in3.3,
themap d
is defined in3.9,
theisomorphism
is as admissible irreducible
weight
1representations
of9(L)
and T is theunique morphism making
thediagram
commute.- -
3.14. DEFINITION
([Mul], Corollary
p.115).
- For alla, b
EQ2’
dehne
The element
b ~ b ~ ]
is in1-lg.
Let a’ E a +Z~
and b’ E b +Z~,
thenIn
particular, (1/2~)Z~
for somenon-negati ve integer
v, then8(~;)
does not
depend
on the choice and2v~2.
Theelements _ _
, , _
/ r ,,,
where a and b are chosen
representatives
inQ~
of the cosetsQ~/71~,
definea basis
of ~ ( r ( L ) ) . Moreover,
the latter is defined in 3.12.
The group
9(&) permutes
the elements of this basis(up
toscalar).
The action is described via the
isomorphism cA in
3.13of 9(&)
~g - ~ib by
3.15. Remark. - In
particular,
the setis the one fixed
by
thesubgroup X§v
defined in 3.5. Remark thatvia the
isomorphism
cA of 3.13. AlsoHence,
a full theta structure defines for eachinteger v
a finite theta structure on(A, pv (,C)~
oftype (22v, ... ~ 22v ~ 22v+1 ~ ... , 22v+1 ).
3.16. Theta characteristics.
Consider the
following
exact sequence:The sequence admits a canonical
right splitting h (as sets!)
The
image
via h of the set defines a choice ofrepresentatives
ofthe cosets defined
by
Call xZg/2’Zg
the set of thetacharacteristics of order
2v .
If(a, b)
are1/2v-theta
characteristics letFinally
call a1 /2"-theta
characteristic(a, b)
even ifx (h(a), h(b)) =
1.3.17. Remark. - If a and b are chosen theta characteristics and 0152
and 0
are inZ~,
it follows from 3.14The group
~(pv,C),
defined in 3.5 and identified in 3.15 withtriples (a,
x,l)
with a in and
(x, l)
in acts as follows:3.18. Remark. - Let w be the element
a a (y)
ofg(£)
with y inV(A)
and a defined as in 3.7. Due to 3.9See 3.12 for the definition of
~9A . Hence,
span the same vector
space v
The two sets are translationsby
elementsof ~ (pv (,C) )
of the element~9A ~o~ _
3.19. PROPOSITION. - Consider two full theta structures
CA
andas in 3.13. The two
corresponding
setsare the same if and
only
the two theta structures of levelinduced on
(A, pv (,C) ) by c~
andc~
as in3.15,
are the same.4. The
Schottky-Jung relations.
In this section we deduce the so-called
Schottky-Jung
relations for smooth curves; see 4.6. We follow the idea sketched in[Mu2].
We assumewe are in the situation of
§1
with 9 =Spec(K)
and K is analgebraically
closed field.
4.1. The
setup
for IThe notations x and
,Cx
are as in 2.3 and in 2.4 with ,S’ =Spec(K).
Since
Lx
is ofdegree 1,
the associated line bundle has aunique
non-zerosection
j3 x
up to scalar. Choose arigidification
of the associated line bundleLx.
Wefreely
use the notation of§3.
Fix a full theta structureand an
element 7/
of such thatIdentify
with itsimage
viaWe have a
surjective morphism
defined
by
where
stands for the restriction toV(X)
via the identification above.Consider the abelian
variety
x with theGm-torsor £x
® Define1. with the notation of 3.5
2. with the notation of 3.10 and of 3.13
for any x in
4.2. Remark. - Recall that the definition of i uses a
normalized
isomorphism 4
, Thenatural choice is that of
where
0: Lx
~[-1]*
a normalizedisomorphism. Indeed,
is the
identity assuring that ~
is normalized.4.3. The
setup
for thePrym variety
P.The notations P and
Lp
are as in 2.14 and in 2.15 with ,S’ =Spec(.K) .
The same
procedure
of 4.1 isapplied
to/~p
andQp
and -Cp.Considering
the abelian
variety P
with the line bundle define:2. for any x in
4.4. The
setup for Y
=The notations
Y
and,Cy
are as in 2.3 and in 2.4 with ,S’ =Spec(K).
By 2.15,
the abelianvariety Y
is aquotient
of x x P and theGm-torsor
descended to
y. Hence,
l.b)
the bilinear form e £y onV(Y)
is definedby
for all
(x, y)
and(a, b)
in xV(P).
There is a
unique monomorphism
such that
)
is contained in theQ2-vector
spaceQ2g-l
xtol
x. the restriction of ex to
preserves the
symplectic
structures and coincides withEp ;
~ the induced
isomorphism
coincides with the
morphism
defined in(5)
of 2.15.Here, fi
standsfor the
orthogonal
inY(X)
withrespect
to thepairing
ex.Then
I , where A
is~
x id. Thisfollows from
2.15;
2.b)
with the identification above the mapef"
onidentified with its
image,
is definedby
4.5. Theta functions on
Pico(C/S),
on and on thePrym variety
P.Choose a non-zero section
j3y
of As in 3.12 wewritedy
insteadof
~,~y .
We use similar notations for the sectionj3 x
defined in 4.1 and thesection
j3p
defined in 4.3.By
2.15 and3.11,
there is a non-zero constantd1
such that for any ain
V(P)
we haveAnalogously,
there is a non-zero constantd2
such that forany b
inY(x)
we have
Equivalently,
due to3.14,
we haveand
Let c be an element of
(1/2)T(~)
and letDefine
c’ :_ ~(c)
E(1/2)T (x).
Thenand
By
HenceBy
3.13and
Hence, by 3.9,
Since
we conclude
by (4.5.1)
andby (4.5.2)
thatOn the other hand we have
by by
(by
(Analogously
and
Hence,
with the notation of3.14,
weget
thefollowing:
4.6. PROPOSITION. - Let
[~] ]
be the setof~-theta
characteristics of P as defined in 3.16.Identify
themwith 1/2 -theta characteristics [a 0] ]
onx via the
map 0
defined in 4.4. Then4.7. COROLLARY. - We have the
following
commutativediagram:
Here
. is the
projective
space in the coordinatesR(a),
b where(a, b)
ranges among all the
1/2-theta
characteristicssatisfying x(a, b)
=1;
. H in stands for the Hurwitz data 7r: C -~ C
given by fixing
the 2-torsion defined in
2.1;
. H in
,~4~4’g~’H
stands for the choice of the theta characteristicappearing
in the definitionProof.
Only
the level structures remain to bejustified.
The use ofthe
(4,8)-level
structures is a consequence of 3.19. The(2,4)-level
structureis motivated
by
thefollowing
remark.4.8. Remark. Let P be a g dimensional abelian
variety
and ,C anample, degree
1 line bundle on P. We have asurjective homomorphism
defined
by (01, ~2 ) F--* 01 (9 02-
Let cp :
V(P) - Q2’
be a full that structure on(P, L).
The vectorspace
spanned by
the theta functionsis an irreductible
weight
onerepresentation
of the As in3.19,
such
representation
defines a level(2,4)-theta
structure on(P, C)-
Conversely given
a level(2,4)-theta
structure on(P, £)
the above setof theta functions is
canonically
defined.5.
Fourier-Jacobi expansion
of
theSchottky-Jung relations.
In this section we
study
theSchottky-Jung
relations defined in 4.6induced to the
boundary.
See the corollaries of5.5,
where westudy
theFourier-Jacobi
expansion
of theta functions. An account on Fourier-Jacobior
q-expansions
can be found in[Ch], §III2,
pp.143-149,
with thewarning
that we use a basis for the theta functions which is different from Chai’s
one. This forces us to go
through
thetheory
to see whathappens
in ourcase.
5.1. A review of some results of Chai.
Let ~
be a rationalpolyhedral
cone contained in0 R;
see[Ch], §II1.2.4,
pp. 146-147. Let v be anon-negative integer.
Let E :=where
~ R is the universal deformation space of a
principally polarized
abelian
variety
with(2 2v 22v ~ 12 2v+l 22v+l )-theta
structureand r marked
sections;
~ a ranges among the
quadratic
forms on(2"~Z~)
so that- the associated bilinear form lies in
~;
- the
element ~ i belongs
to the maximal ideal ofE;
- the
element ~
ifi ~ j ,
is in themaximal ideal of
E;
(Denote by
the associated bilinear form on 2-vZr with coeffi-1
cients in E. It is is
uniquely
defined in terms of the elementsThen, E
is a noetherian excellentdomain, complete
withrespect
to an ideal I and with fraction field K. If v is
positive, Spf (E)
ap-pears as a "chart" at the
boundary
of any toroidalcompactification
of the moduli stacks of abelian varieties with theta structure of level
(2~,.... 2~, 22v+1 ,
7 ...12 2v+l
whose associated conedecomposition
con-tains
~.
5.1.1. The
degeneration
data.Over ,5’ =
Spec(E)
wehave,
as in[Ch], §III.2,
p. 143:1. an abelian scheme B and a
principal polarization
A: B -Bt;
2. an extension G of B
by
asplit
torus T of rank r and character groupX(T).
Denoteby
7r: G - B theprojection
map. Letbe the
morphism
suchthat A oj: X(T) - B’
defines G as an extensionof B
by T;
3. an
isomorphism
Y - (B ’ -’ (BX(T)
as constant group schemes over S’ and a grouphomomorphism
such that the
following diagram
commutes:4. an
ample
line bundleLB
onB, rigidified
above theidentity
elementof
B, inducing
thepolarization
-A.5. a theta structure of level
(22V, ... , 22v ~ 12 2v+l
... ,22v+1 )
on[2V]* (LB );
6. a
symmetric ample
sheaf data a:-1 (8)
withrespect
to t.
5.1.2. The
quotient.
As in loc.
cit.,
we use Mumford’s construction toget
thecouple (X, Lx) consisting
ofi. the semiabelian scheme
X, "quotient"
of Gby Y;
ii. the
ample symmetric
line bundleLx
overX, "quotient"
ofLG
:=7r*(LB) by
Y with- a
rigidification
~po :Lx
above theidentity
element of X)-theta
level structureover the
non-empty
open subset U of S’ where X is an abelian scheme.Denote
by ,CB (resp. £x)
the cubicalGm-torsors
on G(respec- tively X)
associated toLB (resp. Lx);
see 2.8 for this notion.5.1.3.
Properties
of Mumford’s uniformization.For later purposes we note the
following.
DefineG ---> Gi
as the
push-forward
of Gby
the character ei for every i =l, ... ,
r. LetGi (K)
be thecomposition
of l and the natural map G -Gi
Then,
. G x s XQ
as,
where as is thecomplement
of the scheme theoreticimage
ofSpec (.
o the divisor associated to the section
ij (ej)
of thecoincides with the divisor
(q2 i ) ;
. if i
# j ,
the divisor associated to the section of the(Gm,s-bundle j * ( Gi )
coincides with thedivisor (
5.2.
Example:
the case of Jacobians.As an
example,
letCo
be an irreducible semistable curve over k= k
with
singular points Qi , ... ,
Leto V =
Spec(A)
be the universal deformation space ofCo;
o C - V be the
(algebraization of)
the universal(formal)
curve overV;
o for each i =
1, ... ,
r,be the
completion
of C atQi;
~
’ : Spec (A/ (ql , ... , q~. ) ) ;
I~
Dj (resp. D)
be thedesingularization
of C’ := C x v V’along
thesingu-
lar section
of Ci extending Qi
for every z =1,...,
r(resp. Qi , ... , Qr);
~
Pi
andRi
be the sectionsof Dj
overQi
for everyi;
~
Q :
V - C be a smoothsection;
. X :=
PiC°(C/V)j
w
LX
be the line bundle associated to the theta divisor on Xi.e.,
thetranslation of the
image
of inPicg-1(CjS) by - (g - 1 ) Q.
By [FC]
thecouple (X, Lx)
can be "uniformized"i.e.,
obtainedby pulling-back
via V - ,S’(more precisely,
to a cover ofV)
Mumford’sconstruction described in 5.1 for a suitable ,S’
(choosing
a(22v,..., 22v, 2~+B
level structure on[2v]* (x)).
5.2.1.
Properties.
The
following
is known[An]:
1.
2. B x s V’ ^--’
PicO(Ð/V’);
3.
LB
x s V’ is the line bundle associated to the theta divisor of definedtranslating
theimage
of the(g-r-1)th symmet-
ric power of D inPicg-r-1 (ÐjV’) by
thepoint -(g-r-1)Q
XvV’;
4. the character group
X(T)
iscanonically isomorphic
to5. the
map j
x s V’ is defined(up
to a non canonical choice ofsign) by sending Qi
toPi - I~i;
6. the divisor of V associated to the section of the
j * (Gi)
coincides with thedivisor qi
= 0 withmultiplicity 1;
7. if i
~ j,
the elementqi,i qg§
is invertible inV;
8.
Gi
x s V’ ~Pico(Ði/V’).
In
particular,
it follows from 5.1 that6’. the element extends to an element of
Gi
7’. if i
~ j,
the element extends to an element ofGi (V).
Finally,
9. x~ V’ coincides with the difference of
Pj
andRi (as
sectionsof Di ---> V’
5.3. Relations between 2-divisible groups on G and on X via Mumford’s construction.
We use the notations of 3.3 and of 5.1. As
explained
in[Ch], § 111.5,
pp.
69-70,
wehave,
for anynon-negative integer
n, exact sequences:and
r -. ’i B
We have also the exact sequence
In the notations of 3.3 we
get
exact sequences:and
and