C OMPOSITIO M ATHEMATICA
B. D WORK
A. O GUS
Canonical liftings of jacobians
Compositio Mathematica, tome 58, n
o1 (1986), p. 111-131
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111
CANONICAL LIFTINGS OF JACOBIANS
B. Dwork and A.
Ogus
C Martinus Nijhoff Publishers, Dordrecht - Printed in the Netherlands
Introduction
Perhaps
the chief reasonwhy
thestudy
of Fermat curves is sorewarding
is that their Jacobians are of CM
type.
Is there asystematic
way to construct other curves with thisproperty?
In this paper, we examine the limitations of oneapproach
based on ap-adic
method - the "canonicallifting"
of Serre and Tate[15]. They
showed that anordinary
abelianvariety
A over aperfect
field k of characteristic p > 0 has adistinguished lifting Acan
to the Wittring
W ofk;
if k isfinite, A can
is of CMtype.
Thus it is natural to
try
to start with anarbitrary ordinary
curveX/k
and ask if the
canonical lifting
of its Jacobian isagain
the Jacobian ofsome curve. In this paper we show
that, when p
is odd and the genus isgreater
thanthree,
the answer is "no" for most curves, even if one works modp2.
Let us
briefly
sketch our method. We work over analgebraically
closed field k of odd characteristic p ; this allows us to use
crystalline
deformation
theory
togive
acompletely
lineardescription
of the canoni- callifting
of anordinary
abelianvariety.
LetW2 =: W/p 2 W
and letX/k
be a curve of genus g 2 with Jacobian
J/k.
The set ofliftings
ofX/k
to
W2
is a torsor underH1(X, 0398X,k) ~ 0393(X, 03A9X/k),
and the set ofliftings
ofJ/k together
with itspolarization
toW2,
is a torsor underSym20393(X, 03A9X/k).
The cokernelQXlk
of the natural mapcan be
thought
of as the value at X of the normal bundle to the moduli spaceMg
of curves in themoduli
spacef2 g
ofprincipally polarized
abelian varieties. In
(2.4)
we construct an element!3x
ofQXlk
which isthe obstruction we need:
03B2X =
0 iffJcan/W2 is
the Jacobian of a curveover
W2.
Of course, the
key point
is to show that03B2X
isgenerically
not zero.Rather than
try
to constructexamples
for every gand p,
weproceed by
"pure thought".
First we show that the Frobeniuspullback Fk*(03B2X) of /3x
can be
interpolated
in anyfamily
of curvesY/T:
there is a sectionÎ3Y/T
of
F*T(QY/T)
whose value at each closedpointed t
of T isF*k(03B2Y(t)).
Since
QY/T is coherent,
this shows at least that theset 03A3
of all closedpoints
in Tcorresponding
to curves X with acanonical lifting
modp2
isconstructible. When g = 2 or when the fibers of
Y/T
arenonhyperelliptic (as
we maysafely
assume wheng > 2), QYIT
islocally
free of rank(( g - 2)(g - 3)/2),
and then 2 is in fact closed.To show
that 03B2Y/T
is not zero when g 4 andY/ T
is a versalfamily
of curves, we prove that in fact
!3Y/T
cannot be descended tor(T, 6y/r)
r(T, Fj,QY/T)’
This is the same asshowing
that03B2Y/T ~ 0,
where vis the canonical connection which exists on the Frobenius
pullback
ofany coherent sheaf
[10, (5.1)].
Toaccomplish this,
we firstgive
a verysimple
formula(3.2)
for03B2Y/T involving
the Cartieroperator
and themultiplication
map:03BCY/T: Sym20393(Y, 03A9Y/T) ~ 0393(Y, 03A9Y/T).
The rest of our
argument
is clearest if we make a finite étalecovering
of T and choose a level
p-structure
for the Jacobian ofY/T. Using
thewell-known
correspondence
between divisors oforder p
and holomor-phic
differentials fixedby
the Cartieroperator [14],
we find thatr(Y, 03A9Y/T)C
has an(9,-basis f wl,
... ,03C9g},
and the canonical embed-ding
can be viewed as aT-map Y ~ T Pg-1.
Then we seeimmediately
from our formula
(3.2)
that ifi7ÀY/T vanished, KY/T =: ker(03BCY/T)
would also be invariant under the Cartier
operator.
In otherwords,
theintersection
ZYIT
of all thequadrics
inT Pg-1 containing
Y woulddescend to a "constant" subscheme of T. When g
5,
Petri’s theorem[16]
tells us that ageneral
curve of genus g isequal
to the intersection of thequadrics containing it, leading
to the absurd conclusion that thegeneric
curve is definable overFp!
For g =4,
an easy modification of thisargument
can be made to work.It is worth
remarking
that many of ourarguments, including
formula(3.2),
are valid in the context of abstractF-crystals. Consequently they
can also be
expected
toapply
to diversesituations,
such as families of K3surfaces, hypersurfaces,
etc. For the sake of concreteness we have chosen to treat here the case of curvesexclusively, leaving
thegeneralizations
tothe
future,
as need arises.Many
relatedquestions
remain to beinvestigated. Perhaps
the mostobvious is the
problem
ofidentifying
the subsets ofMg/k corresponding
to curves which have canonical
liftings
modhigher
powers of p. Thequestion
ofconstructing nonhyperelliptic
curves ofhigh
genus with CM Jacobians remainsquite mysterious;
mostintriguing
is R. Coleman’ssuggestion that,
forlarge
g, there should beonly finitely
many suchcurves. We also think the moduli of curves with a level p structure, which maps
naturally
to the Hilbert schemeof Pg-1,
warrants further investi-gation.
We had intended to mention theproblem
ofconstructing
"ex-plicit" examples
of curves with nocanonical lifting,
but in fact Oort andSekiguchi have, completely independently,
constructed many such exam-ples [13]. They
were able to conclude that thegeneric
curve of genus ghas
no canonicallifting,
at least wheng 2(p - 1) 8, providing
acompletely
differentproof
of our main result in most cases. We should alsopoint
out that the firstexplicit example
seems to be due to D.Mumford
(letter
toDwork, 1972).
Acknowledgements
We would like to thank R. Coleman for
rekindling
our interest in thequestion
of canonicalliftings
of Jacobians and for several valuable discussions. We also want to thank S. Bloch and his IBM PC for someenlightening computational examples,
as well as G.Washnitzer,
W.Messing,
and Y. Ihara for their interest in this work.§ 1.
Canonicallif tings
of abelian varieties and JacobiansRecall that an abelian
variety
A over analgebraically
closed field k ofcharacteristic p
is said to be"ordinary"
iff it satisfies thefollowing equivalent
conditions:The étale
part
of thep-divisible
group of A is(1.1.1)
isomorphic to (Qp/Zp)g.
The
p-linear endomorphism
ofH1(A, (9A)
inducedby
the absolute Frobeniusendomorphism FA
of A(1.1.2)
is
bijective.
The
crystalline cohomology H1cris(A/W) splits
into a direct sum:invariant under the map
Fl
inducedby FA,
whereFA* U :
U - U is anisomorphism
andF*A|T:
T ~ T is p times anisomorphism.
(1.2)
REMARK: There is a canonicalisomorphism:
which we
permit
ourselves to view as an identification. TheHodge
filtration:
Fil =: F1Hodge ~ H1DR(A/k)
is well-known to be the kernel of theendomorphism HDR( FA)
ofH1DR(A/k)
inducedby FA;
inparticular,
this map
always
has rank g. Itsimage,
often called the"conjugate filtration",
is denotedF1con
cH1DR(A/k).
It is clear that A isordinary
iffthe natural map
is an
isomorphism.
Let
03A6k: F*kH1DR(A/k) ~ H1DR(A/k)
denote the k-linear map corre-sponding
toH1DR(FA). It
factorsthrough
the naturalprojection
F*kH1DR(A/k) ~ F*kH1(A, (!JA)’ fitting
into a commutativediagram
Thus,
A isordinary
iff h isbijective
iff qr isbijective.
When this is the case, the U(resp.
theT )
in(1.1.3)
is theunique H1cris(FA)-invariant
directsummand of
H1cris(A/W) lifting F ôn (resp. FH’.dge).
The letter U stands for "unitroot";
we will also use the notationFilcan
for thesubspace
T.When the context
permits,
we shall also use these notations for the reductions of thecorresponding
spaces modulo various powers of p.Let
Wn
=.W/pnW
and let S =:Spec Wn
orSpf
W. Recall that ifX/S
is any smooth proper formal scheme and
X/k
is its closedfiber,
there isa canonical
isomorphism
compatible
with theisomorphism (1.2.1).
We setIn the absence of
p-torsion
in theHodge
groups, we see thatFilx
is alifting
ofFilx
=:F1Hodge HDR( X/k) to
a direct summand ofHcis(XIS). 1 X/S).
For abelian varieties we
have, since p
isodd,
thefollowing "crystalline
local Torelli theorem"
[11, §5], [2, (3.23)].
(1.3)
THEOREM:If A/k is
an abelianvariety,
the abovecorrespondence (formal liftings
ofA/K
toS }
~(liftings
ofFil A
to adirect summand of
H1cris(A/S)}
is
bijective.
In
particular,
thelifting
T =Filcan
of(1.1)
and(1.2)
defines a formallifting A can
of A toS,
called the "canonicallifting".
This is thecrystal-
line
description
of a famous result of Serre andTate,
who alsoproved
that
A can
is in factalgebraizable.
(1.4)
THEOREM(Serre-Tate): If A/k
is anordinary
abelianvariety,
there isa
lifting Acan/W of A/k
to an abelian scheme overW, uniquely
determinedby
anyof
thefollowing properties:
The p-divisible
groupof Acan splits
as a direct sumof
(1.4.1)
its étale and
connected p ieces. (
There is an
Fwmorphism Fcan: Acan ~ Acan lifting
(1.4.2)
the absolute Frobenius
endomorphism FA Qf A. (1.4.2)
The action
FÂ of FA
onH1cris (A/W)
leavesFilAcan (1.4.3)
invariant.
Moreover
if B/k
is anotherordinary
abelianvariety
the natural mapis
bijective.
Perhaps
the best current reference for this result isMessing’s thesis, especially [11, V, §3
andAppendix]. Although (1.4.3)
is not mentionedexplicitly there,
it followsimmediately
from the methods ofproof.
Onecan also refer to
[2, 3.4]
for anexplicit
discussion of(1.4.3).
Note thatonly
theimplication (1.4.3) ~ (1.4.1)
and(1.4.2) requires
thehypothesis that p
be odd.Moreover,
if k isfinite,
thecanonical lifting Acan/W
isalso characterized
by: End(Acan) ~ End(A) is bijective [11, Appendix, (1.3)].
Note that if A is
ordinary,
so is its dual. One seeseasily
that thecanonical lifting
of the dual of A is the dual of itscanonical lifting.
Thelast
part
of(1.4)
thereforeimplies
that everypolarization
of A liftsuniquely
to apolarization
ofAcan;
this can also be deduced from[2, (3.15)].
Inparticular,
A can is algebraizable.
If
A /S
is any formallifting
of anordinary A/k,
a natural measure ofthe "distance" between A and A
can is
thecomposite
where 71’can is the
projection
associated to the direct sumdecomposition
H1cris
=Filcan
~ U. SinceFilA
andFilcan
areequal modulo p,
we in facthave a map:
This map and its variants will be the
key
to ouranalysis.
Note that TA = 0 iff A =Acan/S.
(1.6)
REMARK:Although
we shall not need it for whatfollows,
it isinteresting
to relate rA to thetheory
of canonical coordinates[5], by
means of
explicit
formulas. Recall from[5]
that the universal formal deformation space T of A over W isformally
smooth of dimensiong2,
and admits "canonical coordinates"
{tlj = qij - 1, 1 i, j g},
withrespect
to which the Gauss-Manin connection looksespecially
nice.Thus,
if
B/T
is the universal formation deformation ofA/k, HbR(B/T)
admits a
basis: {03C91,
... ,03C9j, ~1
...~g} compatible
with theHodge
filtra-tion,
and the Gauss-Maninconnection v
isgiven by:
Moreover,
thecanonical lifting corresponds
to the W-section:{tlj = 0}.
Now any formal
lifting A/S corresponds
to an S-valuedpoint
ofT,
i.e.to a choice of
g2
elements{tij(A)}
of the maximal ideal of(9s.
Thecanonical
isomorphisms H1DR(A/S) H1cris(A/S) H1DR(Acan/S)
canbe calculated
by
well known formulas(cf. [1])
in terms of the Gauss-Manin connection. We find thatSuppose
now thatX/k
is a smoothprojective
curve of genus g 1 and let J =:(A, 0398)
denote the Jacobian of Atogether
with itsprincipal polarization.
There is a canonical commutativediagram:
compatible
with the actions of absolute Frobenius. Inparticular,
A isordinary
iffFx
induces abijective endomorphism
ofH1(X, (9x);
in thiscase one says that X is
ordinary.
It is clear that this conditiondepends only
on theisomorphism
class ofX/k
and henceonly
on theimage
of Xin the coarse moduli space
Mg/k
of curves of genus g over k. It isquite
easy to see that the set
Mg ord(k) of points corresponding
toordinary
curves is Zariski open in
Mg(k);
L. Miller was the first to prove that for every g, it is also dense[12].
If
X/k
isordinary,
letOcan
be theunique lifting
of 8 to the canonicallifting Acan
ofA,
and letJcan(X)=: (can, Bcan)’ a principally polarized
abelian scheme over W. If R is any
W-algebra,
we letJcan/R
denote theprincipally polarized
abelian scheme over R obtained fromJcan by
basechange.
(1.7)
DEFINITION: Anordinary
curveX/k
is"pre-R-canonical " iff
there isa smooth curve
Y/R
whose Jacobian isisomorphic,
as aprincipally polarized
abelianR-scheme,
toJcan(X)/R.
Note that if g
3,
everyprincipally polarized
abelianvariety
of genus g over analgebraically
closed field is the Jacobian of a curve, and that the curve is smooth if the 0-divisor is irreducible.Thus,
if g3,
everyordinary
curve over k ispre-K-canonical.
It
ought
to be clear that thepre-R-canonicity
ofX/k depends only
onthe
isomorphism
class ofX/k.
Thus the class of allpre-R-canonical
curves defines a subset of
Mg ord(k)
which we denoteby 03A3R.
(1.8)
THEOREM:If g 4,
the setLK of pre-K-canonical
curves inJI( g ord(k)
is nowhere dense in
JI( g
ord( k ).
Let
W2
=:W/p2W.
Theorem(1.8)
will followeasily
from:(1.9)
THEOREM: The set03A3w2 of pre-W2-canonical
curves inJl(gord(k)
isconstructible. Its intersection with the
nonhyperelliptic
locus is closed.If
g
4, it is
nowhere dense.Let us
explain
how(1.9) implies (1.8). Clearly
it suffices to prove thatif x ~ Mg ord(k) represents
the class of anonhyperelliptic and pre-
K-canonical curve
X,
then X is also pre-W2-canonical. Suppose Y/K
is asmooth curve whose Jacobian is
J(X)can/K. Necessarily
there is a finiteextension
K’ of K to which Ydescends;
writeY’/K’
for some descent ofY/K.
For K’large enough,
we still haveJ(Y’)/K’ ~ J(X)can/K’.
SinceJ(X)can/K’
has stablereduction,
so doesY’/K’:
there is a stable curveY’ over the
ring
ofintegers
V’ of K’ whosegeneric
fiber is Y’. Thenby [6, (2.5)ff],
the Jacobian of thespecial
fiber of Y’ is thespecial
fiber ofJ(X)can; it
follows that thisspecial
fiberis just
X. In otherwords, Y’/V’
is a
lifting
of X. Let 1 denote the universal f ormal deformation of X and let A denote the universal formal deformation ofJ(X).
Each ofthese is a
formally
smooth formal scheme overW,
and since X is nothyperelliptic,
the natural map ~A is a closed immersion. Thelifting
Y’ defines a V’-valued
point y’
of-IF,
and itsimage
in .91 factorsthrough
a W-valuedpoint.
It follows thaty’
also factorsthrough
aW-valued
point,
i.e. Y’ descends to W. Then ifY/ W
is such adescent, J(Y/W2)~J(X)can/W2,
so X ispre- W2-canonical.
We shall
explain
theproof
of Theorem(1.9)
in the next sections.§2.
Obstructions modp 2
Suppose X/k
is a smoothprojective
curve of genus g. Poincaréduality
in
crystalline cohomology
furnishes us with aperfect alternating pairing:
If e and 1’
are elements ofH1cris(X/W),
one has thecompatibility
relation
One deduces
immediately that,
when X isordinary,
the direct summands U andFilcan (1.1.3)
ofH1cris(X/W)
aretotally isotropic
andmutually
dual.
If
Wn
=:W/pnW
and if X is alifting
of X toWn,
we obtain atotally isotropic lifting Filx
ofFilx
=FI
to a direct summand ofH1cris(X/Wn). By (1.2),
when X isordinary,
the natural mapis an
isomorphism,
since it is modulo p.(2.2)
PROPOSITION:If X/k
is anordinary
curveof
genus g, thefollowing
are
equivalent:
PROOF: If
X/k
ispre-Wn-canonical,
there is a smooth properY/Wn
suchthat
J(Y/Wn ) ~ Jcan/Wn
asprincipally polarized
abelian schemes. Inparticular,
the reduction ofJ(Y/Wn)
to k isisomorphic
to the Jacobianof
X/k,
andby
the Torellitheorem, Y/k
=X/k,
i.e.YI W
is alifting
ofX/k. Thus, (2.2.1) implies (2.2.2).
Theremaining equivalences
are clear.n
Now if
X/W2
is anylifting
ofX/k,
we obtain as in(1.5)
a map:by composing
the inclusion ofFilx
inH1cris(X/W2)
with theprojection
associated with the direct sum
decomposition
Of course,
pF1con
=0,
so TX factorsthrough
Fil x ~ Fil x. In otherwords,
there is a
unique
map:such that for any w E
Fil x,
we havewhere w E
Filx
and ",’ EFilcan
areliftings
of 03C9. It is clear thatX/k
ispre- W2-canonical
iff we can chooseX/W2
such that03B4X
= 0.Recall that the
cup-product pairing
onH1DR(X/k)
induces aperfect pairing (, ) : Fil x X Fcon ~
k.Thus,
we canidentify 8x
with a bilinearmap :
given by: 03B2X(03C9, 03C9’) = 03C9, 03B4X03C9’.
It followsimmediately
from the factsthat (, )
isalternating
and thatFilx
andFilcan
aretotally isotropic
that03B2X
issymmetric.
Thus we canidentify /3x
with a map :Of course,
FilX ~ 0393(X, 03A9X/k),
so there is a natural map(2.4)
PROPOSITION: Therestriction /3 x of 03B2X to ker(ti x)
gSym2 Fil x
isindependent of
thelifting X/W2.
The curveX/k
ispre-W2-canonical iff 18X
= 0.PROOF: Standard deformation
theory
tells us thatDef( X/ W2 ),
the set ofisomorphism
classes oflifting
ofX/k
toW2,
is a torsor under the groupH1(X, (3X/k)’
where of cour-se8X/k
is thetangent
bundle.Moreover,
theset of
liftings Lcris(FilX/W2)
ofFil x
tototally isotropic
direct summandsof
H1cris(X/W2) is
a torsor under(Sym2 Pilx)V (in
the manner describedabove).
We have a natural map of groups:and of sets:
When p ~ 2,
it isproved
in[2, (3.21)]
that the second of these maps is amorphism
over the first one.(For p
=2,
a correction term isrequired [4].)
Inparticular,
ifD ~ H1 (X, 0398X/k)
and ifX’/ W2
is thelifting
obtained from
X/ W2 by "adding" D,
thenFilx,
is obtained fromFilx by "adding" tt’(D).
It follows that we have:If we
identify Cok(03BCX)
withKer(03BCX),
we find that theimage Px
of8x
in this space
depends only on X,
and thatflx
vanishes iff X’ can be chosen so that03B2X’
= 0. D(2.4.3)
REMARK: The restrictionflx
of03B2X
toKer(03BCX)
is an element of the dualKer(03BCX)
ofKer(03BCX),
which we canidentify
withQ x =: Cok(03BCX).
This space has a natural
geometric interpretation:
it is the normal bundle to the deformation space of X in the deformation space to its JacobianJ(X)
as aprincipally polarized
abelianvariety.
Thatis,
we have an exactsequence
(2.5)
VARIANT: We can also use characterization(1.4.3)
to measure howfar
XIW2
is fromdefining
thecanonical lifting. Namely,
letdenote the W-linear map
corresponding
toFi.
If w EF*W FilX, 03A6(03C9) ~
pH1cris(X/W2) ~ H1DR(X/k). Thus,
there areunique
maps:One verifies
immediately
that y x is in fact the inverse transpose of themap D: Fk*Fcon ~ Fcon
inducedby (D (and
hence does notdepend
on thelifting X/W2).
It is well known that this is the inverse Cartieroperator C-1.
It is also immediate toverify
thatIn order to prove
(1.9),
we first show that the obstructions Tx =:Fk*(X)
vary
nicely
in afamily.
To thisend,
letY/T
be a smooth properfamily
of curves of genus g, where
T/W2
issmooth,
and letY/T
be thereduction of
Y/ T
mod p. The yoga ofcrystalline cohomology
thenprovides
us with anF-crystal
onT/ W2 .
For our purposes, we may aswell assume that T is
affine,
so that the absolute Frobenius endomor-phism FT
of T admits(many) liftings
toendomorphisms FT
of T. OurF-crystal
then becomes thefollowing
set of data:- a coherent sheaf of
OT-modules
withintegrable
(2.6.1)
connection
( HT, V).
- a horizontal map:
03A6FT: F*T(HT, ) ~ (HT, V)-
Poincaré
duality provides
us with a horizontalalternating
form:and one has all the
expected compatibilities,
e.g. withspecialization.
Notethat these data
depend only
onY/ T
andFT,
not onY/T.
On the otherhand,
there is a canonicalisomorphism:
under which V becomes identified with the Gauss-Manin connection.
Thus the
lifting Y/T
ofY/T
doesprovide
us with a filtration Fil YHT, lifting
theHodge
filtration onHT = HDR(Y/T).
Assume from now on that each fiber of
Y/T
isordinary.
Then asexplained
in[9]
there is aunique
horizontallifting UT
ofFconT HT to
alocal direct summand of
HT
which is stable under03A6; 03A6
in fact induces a(horizontal) isomorphism ~FT: FT*UT ~ UT.
On the other
hand,
there is no 03A6-invariantlifting
ofFil y,
ingeneral.
The
lifting Fily provided by I’/T will
notusually
beC-invariant,
butwill define a direct sum
decomposition:
Thus,
there areunique
mapsIt is easy to
verify
thatyY,FT
isjust
the inversetranspose
of 03A6:F*TUT ~ UT,
and is thereforeindependent
of theliftings Y/T
andFT
ofYIT
andFT.
We shall denote itsimply by 03B3Y/T.
We shall find it convenient to work with the maps
Our next result expresses the
relationship
between18Y,FT
and the obstruc- tion/3 x
of(2.4).
(2.7)
PROPOSITION: LetQYIT be
the cokernelof
the dualof
the natural mapThen the
image 03B2Y/T of PY,Fr in FT*QY/T is independent of the liftings YIT
and FT of Y /T
andFT.
For anyclosed point t ~ T,
theimage 03B2Y/T(t) of 03B2Y/T in
is
precisely F*k(03B2Y(t)).
PROOF: Associated to each closed
point t
of T is its Teichmullerlifting
t ~
T’( W2 ), uniquely
determinedby
thecommutativity
of thediagram
Via the canonical
isomorphism: t*HT ~ H1cris(Y(t)/W2), t*(03A6FT)
be-comes the
map 03A6: F*WH1cris(Y(t)/W2) ~ H1cris(Y(t)/W2)
used in(2.5).
Moreover, Y(t) =: t*(Y)
is alifting
ofY(t)/k
toW2, and,
via ourisomorphism,
t *Fily
becomesFilY(t) H1cris (Y(t)/W2).
It now followsfrom the definitions that and
The
OT-modules Fily
andr( Y, 03C9~2Y)
arelocally free,
and their formation commutes with basechange.
It follows that the natural map fromQY/T(t) =: t*QY/T to Cok(03BCY(t))
is anisomorphism. By (2.5.3)
and thedefinitions,
we find that theimage
oft*(03B2Y,FT)
inFk*(QY/T(t))
isprecisely Fk*(03B2Y(t)), proving
the lastpart
of ourproposition.
In
particular,
we see that03B2Y,FT(t)
isindependent
of the choicesY/ T
and
FT,
for every closedpoint t
of T. On the open subset of T whereQYIT
islocally free,
atleast,
this isenough
to show that03B2Y,FT
is alsoindependent
of the choices. It is morerevealing, however,
togive
a"crystalline" proof.
First let us
investigate
the effect ofchanging
thelifting Y/T.
Thisinvolves an
argument just
like theproof
of(2.4).
The set of all suchliftings
is a torsor underH1(Y, 0398 Y/T ) ~ 0393(Y, 03A9Y/T). If
twoliftings
Yand Y’ differ
by
an element 0 ofH1(Y, 0398Y/T),
thecorresponding
filtrations differ
by
an element03B2
ofSym2(Fily)V;
infact, 03B2
=03BCY/T(03B8).
Since
FT
is theidentity
map(set-theoretically),
there is a natural map of abelian sheaves:One checks
immediately
thatand hence that the
images
of03B2Y’,FT
and03B2Y,FT in F*T(QY/T)
areequal.
On the other
hand,
the set ofall liftings FT
ofFT
is a torsor underF*T(0398T/k).
IfFT
andFT
are twoliftings, differing by
an elemento E F;«3T/k)’
the yoga ofcrystalline cohomology
furnishes us with acanonical
isomorphism
e:FT*HT FT,HT [1].
Thisisomorphism
can becomputed
from the connection V on the(9rmodule HT. Using
the factthat the divided powers
p[i] = 0 ’a (9T
fori 2,
one findsthat,
forw E
HT lifting w e HT,
Since (D is a
morphism
ofcrystals, 03A6FT,
E =FFT,
so thatSuppose
now that w EFil y,
so that w EFil y.
WriteVia the natural
isomorphism: Fcon ~ HT/Fil y,
the map p becomes identified with the usualKodaira-Spencer mapping [8].
Now let w =:F*T(03C9) ~ F*T Fil y. Using
the obvious abbreviations and thedefinitions,
aswell as the fact that
(DFT : F*T FilY ~ HT
is zero, we find from(2.7.5)
and(2.7.6):
Hence
Of course, the element
is
given by
thecomposite
ofKodaira-Spencer e: 0398T/k ~ Hl(8Y/T)
withcup-product: H1(0398Y/T) ~ Hom(Fily, Fcon) [8]. Using
the notations andidentifications
above,
we can write(2.7.8)
asThis
implies
that the class ofa
modulo theimage
ofF*(03BCY/T)
isindependent
of the choice ofFT,
andcompletes
theproof
of(2.7).
D(2.8)
COROLLARY: The setof
all closedpoints
tof
T such that thefiber
Y(t)/k
is pre-W2-canonical
isequal
to the setof
closedpoints
t such that03B2Y/T(t)=0 in F*QY/T(t).
Inparticular,
it isconstructible,
and it isclosed
if QY/T
islocally free.
nSuppose
now thatT/W2
is the fine moduli space of curves of genus g with level structure andY/T
is the universalfamily.
It is clear that03A3W2 Mg is just
theimage,
via the natural mapT ~ Mg,
of theconstructible set in
Corollary (2.8).
This proves the first statement of Theorem(1.9).
For the second statement, recall that ifX/k
is anonhy- perelliptic
curve(or
if g= 2),
the map03BCX/k
issurjective. Thus,
in thesituation of
(2.7),
if we assume that all the fibers ofY/T
arenonhyperel- liptic (or
that g =2),
we find thatJl y /T
is asurjective
map oflocally
freesheaves. In this case,
QY/T is isomorphic
to the dual of the kernel ofJl Y/T’
and inparticular
islocally
free. This proves the second statement of Theorem(1.9).
We shall prove the third statement in the next section.(2.9)
REMARK:Suppose
thatY/T/W2
is a versalfamily
of curves, i.e.that the
Kodaira-Spencer mapping:
is an
isomorphism.
In this case,F*(QY/T)
is the cokernel of the natural mapWe see from formula
(2.7.9)
that03B2Y/T =
0 iff there exists alifting FT
ofFT
such that03B2FT = 0,
i.e. such thatFily
is invariant under(DFT.
Such alifting FT
is called an "excellentlifting
of Frobenius"[7].
If all fibers ofYIT
arenonhyperelliptic,
or if g =2, 03B2Y/T
= 0 iff each03B2Y/T(t)
=0,
i.e.iff each
Y(t)
ispre-W2-canonical. (In fact,
ifFT exists,
the Teichmullerlifting
of t defines the canonicallifting.)
If X isnonhyperelliptic
andg = 3
(or
if g =2),
the map(2.9.1)
is in fact anisomorphism,
soQY/T is
zero.
Thus,
everynonhyperelliptic
curve of genus 3(and
every curve of genus2),
ispre-W2-canonical,
and there exists aunique
excellentlifting FT
of Frobenius to T. Of course, this is nosurprise, because,
in thesecases, the Torelli
mapping
from T to the moduli ofprincipally polarized
abelian varieties is a local
isomorphism,
and thetheory
of canonicalcoordinates
applies.
§3. Dif f erentiating
the obstructionWe
again
letY/T/W2
denote an affinefamily
of smooth curves of genus g 4 andY/T/k
its reduction mod p. In this section we shall provethat,
ifY/T
isversal,
itsgeneral
member is notpre- W2-canonical,
i.e.03B2Y(t)
~ 0 forgeneral
t. Now we have shownthat {F*k03B2Y(t): t ~ T}
can be"interpolated":
there is a section03B2Y/T of F*T(QY/T)
whichspecializes
ateach t to
F*k03B2Y(t).
We shall in fact seethat {03B2Y(t): t ~ T}
cannot beinterpolated,
i.e. the element03B2Y/T
ofr(T, F;QY/T)
does not lie in thesubspace r(T, QY/T).
Of course, thisimplies
that it is not zero!As is well
known,
for anyquasicoherent sheaf Q
on any smooth k-schemeT,
the sheafFTQ
has a canonicalintegrable
connection v, characterizedby Q
=Ker(FT*) [10]. Thus,
what we must show is that for a versalfamily Y/T/k,
the element03B2Y/T
OfF;QY/T
~2TIk
is notzero. As a first
step,
wepresent
asimple
formula for this element. It isimportant
to note that theproof
of our formula ispurely formal,
and inparticular
would make sense in the context of abstractF-crystals.
In order to write our formula in the most
elegant form,
we assume thatthe
family Y/T
isversal,
i.e. that theKodaira-Spencer mapping 0398T/k ~ H1(Y, 0398Y/k)
is anisomorphism.
We thenidentify (3Tlk
withH1(Y, (3Y/k)
and
0
withr( Y, 03A9Y/T). Thus,
weregard JLY/T
as a map:Recall
again
thatJ.LY/T
can becomputed
from the Gauss-Manin connec-tionv and the bilinear
form (, )
onH1DR(Y/T) by:
Let us also assume that all the fibers of
Y/T
arenonhyperelliptic,
sothat
ftYlT
issurjective,
and letThus,
our obstruction can beregarded
as a(9,,Iinear
map(3.2)
PROPOSITION: Let v:F*T(QY/T) ~ 2 Tlk
~FT(QY/T)
be the canoni-cal connection described
above,
letf3Y/T
EF*T(QY/T)
be the obstruction(2.7),
and let y:F*TFilY ~ Fily
be the inverse Cartierisomorphism (2.6.5) (the
inverse transposeof Hasse-Witt).
Then thefollowing diagram
iscommutative:
PROOF: Let
H =: HT, together
with itsintegrable
connection p, and let U =:UT ~ H,
Fil =:FilY ~ H.
Since U H is invariantunder
theconnection p,
thequotient
moduleH/U
inherits aconnection
p.Using
the natural
isomorphism:
Fil- H/U,
we canregard V
as a connectionon
Fil,
which we denoteby
a. Note that Fil ~ H is not invariant under V; infact, (with
the obviousnotations),
"is" the
Kodaira-Spencer mapping. Thus,
We can view
’Fil:
Fil H and U: H - U as maps of modules withintegrable
connection.Using
the usual conventions for the induced p onHom’s,
we find:Now let
FT:
T - T be alifting
of.FT
and(H, V, û, Fil)
=:F*T(H, , U, Fil).
We have a horizontalmap 03A6=: 03A6FT: (H, , Û) -
(H,
,U),
and thecomposite U 03A6 iFil,
"dividedby p "
is ourobstruction
aFT.
We calculate:Here
p:
Fil -03A9T/W2
0U
is the map defined as in(3.2.2);
one checkseasily that p
=d FT F*T(03C1)
and hence is divisibleby
p. Recall that~:
U ~
U is theisomorphism
inducedby 0,
and that03B1Y,FT = ~-1
oO:y ’ F . T Thus,
if we let~FT: F*T03A9T ~ 0 T
denote the map inducedby p-1 dFT,
wefind the
following
formula:Since our
pairing Fily
XFcon ~ (9T
ishorizontal,
we have the formula:But ~
is the inversetranspose
of y, and(via
the identification(3.1.1)),
the bilinear form induced
by
p isjust 03BCY/T.
Thus we haveproved:
In other
words,
thefollowing diagram
commutes:We should
perhaps
remark that11FT depends
on theliting FT
ofFT,
butthat it factors
through
the closedone-forms,
and itsprojection
toH1(03A9T/k)
isjust
the inverse Cartieroperator [1, §8].
At any rate, this term is no immediate concern to us, because of courseF*T(03BCY/T)
vanisheson
FT*(KYIT). Thus,
thediagram (3.2.9) specializes
to our desired for-mula
(3.2.1)
when we restrict toFj,(KY/T)’
The
following
resultcompletes
ourproof
of Theorem 1.9.(3.3)
THEOREM: LetY/T be a
versalfamily of nonhyperelliptic
curvesof
genus g 4. Then
~03B2Y/T
is notidentically
zero. In otherwords, 03B2Y/T
doesnot descend to a section
of QYIT-
PROOF: Recall that we have an exact sequence
By (3.2),
we seethat -B1Î3Y/T
can be viewed as thecomposite
map:Here y is the inverse Cartier
operator. Thus,
if~03B2B/Y=0, KYIT
isstable under y. We shall see that this is
impossible. Indeed,
for any curve X of genus g1,
the linearsystem Fil x = r( X, ax)
is basepoint free,
and there is a canonical map
When X is
nonhyperelliptic,
this map is a closed immersion. If we letPFily
denote theprojective
bundle over T associated to thelocally
free(9,-module Fily,
weget
a closed immersion of T-schemesNow
Fily
has no canonicalbasis,
but it comes close tohaving
acanonical
Fp-lattice, provided by
theisomorphism
y:FT* Fil, - Fil y.
Namely,
after T isreplaced by
a finite étalecovering,
the sheaf ofFp-vector
spacesFily
=:( w (E Fil y: y(1
~03C9)
=03C9}
spansFil y,
and in fact the canonical mapis an
isomorphism. (This is just Lang’s theorem.) Thus,
ifP(Fil03B3)
is theprojective
space overFp
associated toFil03B3,
we have a canonical isomor-phism :
T XP(Fily) P(Fil y). (We
could even choose a basis ofFil,
and write
P(Fil)
~fFDg-l;
such anisomorphism
would beunique
up to the action of thefinite
groupPGL( g, Fp).
Ourmap 03C8Y/T
then becomes amap of T-schemes:
Recall that
03BCY/T: Sym2 FilY ~ QT/K is
identified withmultiplication Sym2 FilY ~ r( Y, 03C9Y2). Thus,
its kernelK Y/T is just
the set ofquadratic
forms which vanish on
Y,
and thecorresponding
divisors areprecisely
the
quadrics
in TP(Fil03B3)
which contain Y. IfKY/T is
invariant under y, thesubspace K03B3 =: {03C9 ~ KY/T: 03B3(1 ~ 03C9) = 03C9} = K ~ Sym2(FilY)
de-fines an