Maths > Abelian varieties > Absolute Hodge classes
Hodge classes on abelian varieties
Posted by Martin Orr on Monday, 25 August 2014 at 18:50
In this post I will define Hodge classes and state the Hodge conjecture. I will restrict my attention to the case of abelian varieties and say the minimum amount necessary to be able to discuss the relationships between the Hodge, Tate and Mumford-Tate conjectures and absolute Hodge classes in subsequent posts. There are many excellent accounts of this material already written, which may give greater detail and generality.
Hodge classes are cohomology classes on a complex variety which are in the intersection of the singular cohomology 
and the middle component 
of the Hodge decomposition

They can also be defined as rational cohomology classes which are eigenvectors for the Mumford-Tate group.
The Hodge conjecture predicts that these classes are precisely the 
-span of cohomology classes coming from algebraic subvarieties of 
.
Note: Hodge classes are usually defined as living in the Tate twist rather than in the cohomology group 
itself.
This is because the cycle class maps for singular and for de Rham cohomology differ by factors of 
, as explained in my post on Tate twists.
In this post, I shall only consider the singular cohomology normalisation of the cycle class map and hence omit Tate twists.
Hodge structures and
of an abelian variety
So far in this blog, I have talked a lot about the homology group
of an abelian variety and its Hodge structure.
I also briefly mentioned the cohomology group
when talking about Hodge symplectic forms.
Now I need to talk about the cohomology groups
in general.
Let's start with
, which is the dual of
.
Recall that
is a free
-module of rank
.
The Hodge decomposition
induces a decomposition

where

and likewise for 
.
We could call this type of structure an
-Hodge structure.
(The precise definition is the
case of the definition below.)
It is also known as an effective
-Hodge structure of weight
.
Hodge structures and higher cohomology of abelian varieties
We can generalise the above concept to an effective
-Hodge structure of weight
.
This is defined to be a finite-rank
-module
together with a decomposition into complex vector spaces
satisfying 
for all
and
.
(The word effective means that we only have pieces
where
.
The words weight
mean that for every piece,
.)
The importance of this concept comes from the fact that for every smooth projective complex variety
(and more generally for every compact Kähler manifold, which includes all complex tori), the cohomology group
comes with an effective
-Hodge structure of weight
.
I will not discuss the general construction here, but I will discuss what these Hodge structures are in the case of abelian varieties.
The complex abelian variety
is homeomorphic to the product of
circles.
Basic topology gives us that the cohomology groups are the exterior powers of
:

Given an effective Hodge structure
of weight
, we can make its
-th exterior power into an effective Hodge structure of weight
by using the decomposition
It turns out that

is indeed the correct Hodge decomposition for 
of an abelian variety.
Hodge classes
Let us consider the intersection
We have already seen this in the case 
, where we called elements of this intersection Hodge symplectic forms.
If
then this intersection is
.
This is because each element of
is fixed by complex conjugation, so
But 
is zero whenever
because
and the Hodge decomposition is a direct sum.
On the other hand, when
, we have
and so
may be non-zero.
We call elements of
integral Hodge classes of weight
.
In an earlier post, we essentially defined a Hodge symplectic form to be an integral Hodge class of weight 2. Hence the existence of a polarisation (a Hodge symplectic form satisfying a positivity property) guarantees that an abelian variety possesses a non-zero integral Hodge class of weight 2. The group of integral Hodge classes of weight 2 is known as the Neron-Severi group and its rank, called the Picard number, is an interesting invariant of the abelian variety.
In these blog posts, it will be more convenient to work with
We call elements of this group Hodge classes of weight 
.
(Sometimes people call these elements rational Hodge classes, and use the term Hodge class to mean what we call an integral Hodge class.)
Algebraic cycle classes and the Hodge conjecture
The Hodge conjecture is not part of the main things I intend to write about in this blog, but I feel that I should not talk about Hodge classes without mentioning it briefly. It also provides motivation for some of the things we do with Hodge classes, and indeed give one reason why we care about Hodge classes in the first place.
Let
be any smooth projective complex variety.
If
is a complex algebraic subvariety of codimension
, then we can use Poincaré duality to define a class
in
.
It turns out that
is always an integral Hodge class.
A class in
is called an algebraic cycle class if it is in the
-span (or sometimes the
-span) of those classes of the form
.
The Hodge conjecture states that every Hodge class is an algebraic cycle class.
Hodge conjecture. The classes
of algebraic subvarieties of
of codimension
span the
-vector space
.
Hodge classes and the Mumford-Tate group
We can give a characterisation of Hodge classes using the Mumford-Tate group. The key reason why this is important is that there is a sort of converse which I will discuss in a subsequent post, using Hodge classes to characterise the Mumford-Tate group.
Let us recall the definition of the Mumford-Tate group.
Associated with the
-Hodge structure
, there is a group homomorphism
such that
acts as multiplication by
on
and by
on
.
The Mumford-Tate group of
is defined to be the smallest algebraic subgroup
defined over
and such that
contains the image of
.
For each
, there is a standard representation of
on
.
We can compose these with
from the previous paragraph to get homomorphisms
If we look at the eigenspaces of these homomorphisms, we find that 
acts as multiplication by
on
.
Hence
is the subspace of
on which
acts as
for all
.
We would like to state this in terms of the Mumford-Tate group instead of
, so we proceed as follows.
The image of
(and hence also the Mumford-Tate group) is contained in the group
consisting of elements which preserve the symplectic form
associated with a chosen polarisation (up to scalars).
There is a character
defined by

The fact that
is a Hodge symplectic form implies that
.
So
acts on
as multiplication by
.
For each Hodge class
of weight
, consider the algebraic group
This group is defined over 
, and by the above its real points contain the image of
.
Hence
contains the Mumford-Tate group of
, and thus all of
acts on
as multiplication by
.
On the other hand, if we have some
which is an eigenvector for all of
, then it must in particular be an eigenvector for
.
We know that the eigenspaces of
on
are precisely the pieces of the Hodge decomposition, and the only such piece which can intersect
is
.
Thus any eigenvector for
must be a Hodge class.
We deduce that
Proposition. A class in
is a Hodge class if and only if it is an eigenvector for the action of
.
.