C OMPOSITIO M ATHEMATICA
J. H. S AMPSON
Higher jacobians and cycles on abelian varieties
Compositio Mathematica, tome 47, n
o2 (1982), p. 133-147
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133
HIGHER JACOBIANS AND CYCLES ON ABELIAN VARIETIES
J. H.
Sampson
© 1982 Martinus Nijhoff Publishers - The Hague
Printed in the Netherlands
Aldo Andreotti In Memoriam
1. Introduction
A
long outstanding problem
in the transcendentaltheory
ofalgebraic
varieties is to find a
cohomological
criterion for acycle
on analgebraic variety
to be itselfalgebraic (see Hodge [3], Chapter 4).
Criteria areavailable in certain cases; but
they
are far fromcomplete.
Because of the
sensitivity
of abelian varieties tomoduli, they
offer anattractive terrain upon which to test the so-called
"Hodge conjecture"
concerning
the connexion betweenalgebraic cycles
and real harmonicforms of type
(p, p)
withintegral periods.
Forsufficiently general
abelianvarieties,
asexpressed by
suitableindependence
of theperiods
in a nor-malized
period matrix,
theHodge conjecture
is known to be true(Mattuck [7],
Comessatti[2]).
Here we show that the
problem
can be related to A. Weil’shigher
Jacobian varieties. For odd p, the
p-th higher
JacobianÂ
of an abelianvariety
A turns out to admit ahomomorphism
rc onto A. We computeexplicitly
the kernel K of n and theresulting splitting
ofÂ.
We thenshow that to any real harmonic form 9 of type
(p, p)
withintegral periods
on A we can associate a real(1, l)-form
withintegral periods
onÂ.
In this way it ispossible
to define analgebraic (divisorial)
corre-spondence
between A and the kernel K, from which we are able to obtain variousalgebraic cycles
on A associated with the form (P.However,
their connexion with ç is ratherobscure,
because of thehighly
transcendental nature of ourconstruction,
and we have not yet succeeded inmaking
thecomputations
needed toclarify
it.Some of our
results, especially concerning
n, were obtained ca. 1960.0010-437X/82080133-15$00.20/0
2.
Ingredients
The materials
required
for apolarized
abelianvariety
over the com-plex
field C are as follows(cf.
Weil[11], [12]) :
a real vector space Y ofeven
dimension,
say2n;
a latticeL c Y,
i.e. a discretesubgroup
of rank2n;
anendomorphism
J of V such that J2= - Id;
analternating
bilinear form E : V x V - R
(real field)
such thatE(u, v)
isintegral
for allvectors u, v in
L and, finally,
such that the bilinear formQ(x, y)
= E(x, Jy)
on Y issymmetric
andpositive
definite.V is then made into a
complex
vector spaceby defining
ï x = Jx(i = / Î);
andH(x, y)
=Q(x, y) -
i -E(x, y)
is an Hermitian metric on V It induces aHodge
metric on thequotient, A
=Y/L,
whichthereby
becomes a
polarized
abelianvariety.
H is called a Riemannform
for A(but terminology
is rathervariable).
Observe that
E(Jx, J y)
=Q(Jx, y)
=Q(y, Jx)
=E(x, y).
3.
Subspaces
In the
sequel
we shallrequire only
aspecial
case of thefollowing elementary
result.Let el, ..., e2n be a base for
L,
and let U be thesubspace
of Vspanned by linearly independent
vectors u1,..., um, with say ua =uej (sum-
mation convention here and
elsewhere).
PROPOSITION 1: U n L has rank m
if and only if there
is a number c :0 0 such that c. D isintegral for
every m x m minor Dof
the matrix u =(ul,
PROOF: If U n L has rank m, then there is a
non-singular
matrix a= (ap)
such thatIf u’ is an m x m submatrix of u, then u’a is
integral,
and so(det u’)(det a)
is an
integer.
For the converse, let c. det u’ E Z for all such u’. Write u, with
possibly permuted
rows, aswhere u" is of size 2n x m.
Assuming
det u’ =1=0,
let v be the inverse of u’.If u’ denotes the k-th row of u, then
Uk = plul + ... + pmu’"
for certain numbers pa. Nowreplace row j
of u’by tA
The determinant is then Pj. D, where D = det u’.By assumption,
c times this determinant is in-tegral,
i.e.We have
and so
Finally,
cD isintegral,
and therefore so is ua, where a = cDv.Q.E.D.
If U satisfies the conditions of the
proposition
and is moreover stableunder the operator
J,
thenU/ U
n L has an induced structure of abeliansubvariety
of A.4.
Higher
JacobiansLet p be an odd
integer
2n(later
we shall want 1 pn).
Formthe exterior
products
and let
L
denote the latticegenerated by
the elementswhere
again ei
is a base for L. I is the multi-index I =(il,.", ip)
with1
ïi
...ïp
2n.Next, writing
x = Xi A ...A Xp, y = Yl
A ... A Yp, we setand we have
If ul, ..., u2" is an orthonormal basis for V relative to the form
Q,
then(Here
and below we use J both for thecomplex
operator in V and as a multi-index. No confusion canpossibly result.)
From
§2
and theforegoing
we have thus obtained a newpolarized
abelian
variety
which can be identified with Weil’s
p-th
Jacobian of A(cf. [10]).
5. The
homomorphism
Again
let el, ..., e2,, be a base for the latticeL,
and introduce real coordinates x in V or Aby
x --+xiei.
From the Riemann form E weobtain the differential 2-form
Write and build the
2q-form
where
Let Aij denote the cofactor of aji. Thus
where a =
(aij).
Setand define n :
9- V by
Here and
below,
I =(i1, ..., ip)
withil
...i p,
etc.Since
the ai
areintegers,
this map carriesL
into L and so induces ahomomorphism,
still called n, ofÂ
to A.It is easy to
verify
thefollowing
fact:PROPOSITION 2:
If n’: P -+ V is the homomorphism defined
in ananalog-
ous manner
starting from
any basis vl, ..., V2nof V,
then n’ =(det c)2n,
where vi =
de.
and c =(cij).
In
particular,
if{Vi}
is a new base forL,
then the matrix c is un-imodular,
and so then n’ = n.PROPOSITION 3: n is
surjective.
PROOF: Let
{e’i}
be asympletic
basis for Y:By Prop.
2 we haveonly
to show that thehomomorphism
n’ con-structed from
(e§)
issurjective.
We introduce real coordinates(y’) by
y -+
y’e.
Thenwhere we write
It will also prove convenient to write
and
for a multi-index
We have
where
again q
=2(p
+1);
and sobit ...ip having
the value ± 1 if{il,.", ip+ 1}
={iT,..., i;+ 1}
and if thereare no
repeated
indices. Otherwisebil...ip
= 0. In the indexequality
wemean that the set
{i1, ..., ip+ 1}
is invariant under the involution i - i*. Ifnow Bjk is the cofactor of
bkj
=E(ei, e’j),
we haveAccordingly
thehomomorphism
n’ isgiven by
Fix k and take
For this I,
bj
= 0unless j
= k. It is then clearthat ek
occurs in theimage
of7rB
hence also of n.Q.E.D.
PROPOSITION 4: n is C-linear.
PROOF:
Again
let{ei}
be a base for L and writeThen
Next,
and
We must show that
Multiply
both sidesby
aki. SinceA’‘aki = - (det a)àl,
the left side isThe
right
side isMultiply
both membersby h p + 1:
We must show thatObserve that
Now the left side of the
previous equation
can be writtenwhere s runs
through
thepermutations
of{ 1, ...,
p +1}. By
the remarkabove,
this reduces to6. A
special
baseWe now fix a
quasi-symplectic
base ei in L for the form E. Thatis,
forwhere
the di
areintegers
such thatd11d21...Idp; viz., they
are the elemen- tary divisors of E(cf. Siegel [9],
p.65).
For indices n +1,...,
2n we writeAs
before,
we introduce coordinates x’ in Vby
x -x’ei,
andsimilarly
X’
in 9 by xl el.
Thatbeing
so, we can writewhere aij = 0 if j :0 i*,
and aii. =di. Similarly, on 9
we haveHere
âI f
= 0 if JI*,
andà,,. = dl
=dit ... dip. Indeed,
theproducts
el = eh A ...
A eipyield
aquasi-symplectic
base forL:
where 1 = number of i n in 1.
7. The kernel of 1t
We continue with the notation of
§3,
but henceforth referred to thequasi-symplectic
base{ei}
of thepreceding paragraph.
Thenn(ei)
=
aÎek,
and it follows from theproof
ofProp.
3 thata§
= 0 unless alk* has a set lk*of
p + 1 distinct
indices,
invariant under *.Call an index l
"good" (1
eG)
if 1contains p 2 1
distinctpairs i
i*and one
index,
denotedby p(I),
different from all of those. Otherwise write 1 E B("bad").
If1 E B, then aÎ
= 0 for all k.For k =
1,...,
2n we now letÀ(k)
denote an index J =Ub...,jp)
in Gwith
p(J)
= k and with maximum absolute value ofWe can
clearly
do that in such a way thatA(k*) = Â(k)*. Finally,
welet
Go
be the set ofgood
indices 7 such that 1 =F,(p(1)).
Thatbeing
fixedwe have
PROPOSITION 5: W = Ker n :
V -+ V
isspanned by
the elementswhere mi is a
product
of certaindj.
PROOF: For bad
I, n(e¡)
=0,
asalready pointed
out. For 1E Go, 7r(ej)
aJIe. i
andir(eÂ,(,»
=a{p(j).
Letp(I)
= k. Then as remarkedabove,
n(ej)
=a’ek (no
sum onk);
andir(eÂ,(,»
=a k.(,)ek.
From the definitions and the fact thatdjid2i... Id, it
followseasily
that the coefficients hereare both
products
ofdj’s,
and that the latter islarger than aÎ
in absolutevalue,
hence is divisibleby aj.
The elements
(i), (ii)
areobviously linearly independent. V
bas dimen-sion) ,
and the number of elements(i), (ii)
isclearly
2n.Then
Prop.
5 follows from the fact that n issurjective. Q.E.D.
Let K denote the kernel of n :
 --+
A. Then K is an abeliansubvariety
of
Â,
hence has the formThe elements
(i), (ii)
are inL and consequently
generate a sub-lattice L ofL
of finite index in W nL.
Then the abelianvariety
is a finite
covering
of K.8.
Splitting
ofÂ
W
being
as above the kernel of n :9 - E
let U denote theorthogonal complement
ofY
with respect to the formÊ
of§4.
If x E U, so that
Ê(x, W)
=0,
thenTherefore U is a
complex subspace of Ç: Further,
if x E Un W,
thenJx
E W, and soÊ(Sc, Jx)
=0,
i.e.ù(k, x) = 0,
whence x = 0. Thus9
= U+ W
(direct sum).
Thissplitting
leads to asplitting of Â
in accordancewith the
"complete reducibility
theorem" of Poincaré(cf.
Weil[12], Chapitre VI,
no.11,
Théorème6).
Here we shall make thisexplicit (cf.
§2, Prop. 1).
For k =
1,...,
2n setwhere
and where
(see Prop.
5 fornotations).
Observe thatC;k)*
= 1.PROPOSITION 6: The elements
ék form
abasis for
U.PROOF: For I e B it is clear that
Next take 1 E G with
p(I)
=k,
I *Â(k).
Thatis, 1 E Sk.
Then it isplain
that 1 -#
Â(k)*.
We have(cf. Prop. 5)
The first two terms
vanish;
the last two reduce toHence
the ëk
areorthogonal
to the kernel of rc.They
areobviously linearly independent,
which establishes theproposition. Q.E.D.
It is evident that the
elements ék
are inL. They
therefore generate a sub-latticeLo
of rank 2n contained in U. Thus U nL
has rank2n,
andaccordingly
we have an abeliansubvariety
in Â
and a finitecovering
of A’. Via n, A’ is a finite
covering
of A, and therefore so is B.Write
Then
where hk
is aninteger 0,
andBut
aj ,Z(k)
= 0unless j
=k*,
and so we havethe pk being
non-zerointegers.
9. Forms of type
(p, p)
Let vl, ..., Vn be a
complex
basis in V. We introducecomplex
coor-dinates za
= Ça
+i11a by
z -z"va.
And we now assume that the odd in- teger p is n. A harmonic(p, p)-form 9
on A has anexpression
where the coefficients are constants. We assume that qJ is real: qJBÃ =
-(oAÈ.
We assume further that all of theperiods
of ç areintegral.
We now define a bilinear form 0
on ÿ by
where
7§j
is the oriented torusgenerated by
eu , . - .,eip’
eh’...’ejp’
the eias in
§7.
It is well known that thecycles Tjj
with I n J = 0 generate theintegral homology
of A in dimension2p (cf.
Lefschetz[6], Chapitre 6,
No.
6).
PROPOSITION 7:
If qJ -# 0,
then the bilinearform 0
onV
is not the zeroform.
It isalternating
and hasintegral
values onL.
Moreover, it isof
type(1,1).
PROOF: The first assertion follows from the
preceding remark; 0
isalternating
because JI is an oddpermutation
ofIJ;
it isintegral
onL
xL
because of ourassumption
that ç hasintegral periods.
We comenow to the last
point.
Set
Then
where
(xi)
is the real coordinate system on V definedby
the basis{ei}
(see §6).
Foruniformity
ofnotation,
let J =(ip 11, - - -, i2p).
ThenThen
But
(cf. §5),
and soQ.E.D.
W defines a harmonic differential
form 0
of type(1,1)
onÂ
whoseperiods
are thequantities tPIJ
=0(ej, ej).
In terms of the real coor-dinates x, on
 (or V),
It should be noted that we have not
attempted
to associatecomplex
coordinates
in 9
with the z" in VPROPOSITION 8:
If the form
ç ispositive,
then so is0.
PROOF: ç is
positive
if the hermitian formis
positive,
which we now suppose. ThenHere
and
From the
expression
exhibited above for0(ej, je.)
we obtainwhich is
positive,
for thedecomposable
vector x. If wereplace
xby
x+
, writing yi
=Ylej
=w"v,,,,
then in the determinant abovezf
will bereplaced by zf
+wf,
and the same conclusion obtains. The assertion followseasily
for anarbitrary
elementof P
different from zero.Q.E.D.
Of course in
general (p
will not bepositive;
but for a suitableinteger
bthe form ç + bmP will be
positive.
10.
Algebraic cycles
The construction of the
preceding paragraph provides
us with an iso-morphic mapping,
call itf,
from the groupFp
of real harmonic(p, p)-
forms 9 with
integral periods
on A into the group of real(1, 1)-forms 0
with
integral periods
onÂ.
We recall that anyalgebraic cycle
of(real)
dimension 2n -
2p
on A(more precisely,
itshomology class)
is dual tosuch a
(p, p)-form
9, and so the group of realhomology
classesGp
ofsuch
cycles
is embedded inFp, by duality.
On the other
hand, 0
=J(qJ)
is dual to a class of(2N - 2)-cycles
on (N
=complex
dimension ofÂ),
and the class contains analgebraic cycle (divisor).
If D is such adivisor,
then D establishes analgebraic
corre-spondence
between A and the kernel K of n(cf. [1, Chapter 6], [4,
BookIII, Chapter XI]
and§7 above).
Let Z denote analgebraic cycle
on K ofreal dimension
2r,
and putZ = n -1(Z).
Then the divisor D can be sotranslated in
Â
that the intersection D.Z
is defined. Itsprojection
in Ais then an
algebraic cycle ZA
of dimension 2r - 2(which
we assume ofcourse to be -
2n),
or else is zero. In this way we obtainalgebraic cycles
of various dimensions in A.
As we are concerned here with
cycle
classes with respect to real ho-mology,
the aboveopérations
can be taken in thehomological
sense.Thus,
if ÔJ is the fundamental Kähler( 1,1 )-form on Â
and roK is theinduced form on K, the class dual to
CON’-,, (N’ =
dim K = N -n)
con-tains an
algebraic 2r-cycle
Z(intersection
of divisors onK).
ThenZ
isdual as
cycle
to somemultiple kÔJN’-r.
The harmonic form on A dual to theprojection ZA
is then obtainedby integration
of this latter form overthe fibres of n :
 -
A.In
particular,
for suitable r we get ahomomorphism f *
fromFp
toGp.
Despite
the veryexplicit
nature of thecalculations,
orperhaps
because of
it,
i.e.using
the results of§§7, 8,
it seemsquite
difHcult toclarify
the connexion between/*(?)
and 9. If however it could be shown thatKer f *
=0,
then fromsimple
rank considerations we could infer that our(p, p)-form
ç is dual to a class c such that somemultiple
kccontains an
algebraic cycle.
11. Remarks
In the
foregoing
p wasalways
taken to be an oddinteger.
Weil’shigher
Jacobians for even p are definedby
means ofduality
of abelianvarieties. But with reference to forms of type
(p, p),
for even p it wouldseem more to the
point
toreplace
çby
9 A ro orby Alp (ll
as in[12]).
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[3] W.V.D. HODGE: The Theory and Applications of Harmonic Integrals. Cambridge,
1952.
[4] W.V.D. HODGE and D. PEDOE: Methods of Algebraic Geometry. Cambridge, 1946.
[5] S. LANG: Abelian Varieties. Interscience, New York, 1959.
[6] S. LEFSCHETZ: L’Analysis Situs et la Géométrie Algébrique. Paris, 1950.
[7] A. MATTUCK: Cycles on abelian varieties. Proc. Amer. Math. Soc. 9 (1958) 88-98.
[8] D. MUMFORD: Abelian Varieties. Oxford, 1970.
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[10] A. WEIL: On Picard varieties. Amer. J. Math. 74 (1952) 865-893.
[11] A. WEIL: Théorèmes fondamentaux de la théorie des fonctions thêta. Sém. Bourbaki
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(Oblatum 22-1-1981) Dept. of Mathematics
The Johns Hopkins Univ.
Baltimore, MD 21218 U.S.A.