Trace field of a representation explained
In mathematics, the trace field of a linear group is the field generated by the traces of its elements. It is mostly studied for Kleinian and Fuchsian groups, though related objects are used in the theory of lattices in Lie groups, often under the name field of definition.
Fuchsian and Kleinian groups
Trace field and invariant trace fields for Fuchsian groups
Fuchsian groups are discrete subgroups of
. The trace of an element in
is well-defined up to sign (by taking the trace of an arbitrary preimage in
) and the
trace field of
is the field generated over
by the traces of all elements of
(see for example in).
The invariant trace field is equal to the trace field of the subgroup
generated by all squares of elements of
(a finite-index subgroup of
).
The invariant trace field of Fuchsian groups is stable under taking commensurable groups. This is not the case for the trace field; in particular the trace field is in general different from the invariant trace field.
Quaternion algebras for Fuchsian groups
Let
be a Fuchsian group and
its trace field. Let
be the
-subalgebra of the matrix algebra
generated by the preimages of elements of
. The algebra
is then as simple as possible, more precisely:
If
is of the first or second type then
is a
quaternion algebra over
.
The algebra
is called the quaternion algebra of
. The quaternion algebra of
is called the
invariant quaternion algebra of
, denoted by
. As for trace fields, the former is not the same for all groups in the same commensurability class but the latter is.
If
is an
arithmetic Fuchsian group then
and
together are a number field and quaternion algebra from which a group commensurable to
may be derived.
Kleinian groups
The theory for Kleinian groups (discrete subgroups of
) is mostly similar as that for Fuchsian groups. One big difference is that the trace field of a group of finite covolume is always a number field.
Trace fields and fields of definition for subgroups of Lie groups
Definition
When considering subgroups of general Lie groups (which are not necessarily defined as a matrix groups) one has to use a linear representation of the group to take traces of elements. The most natural one is the adjoint representation. It turns out that for applications it is better, even for groups which have a natural lower-dimensional linear representation (such as the special linear groups
), to always define the trace field using the adjoint representation. Thus we have the following definition, originally due to
Ernest Vinberg, who used the terminology "field of definition".
Let
be a Lie group and
a subgroup. Let
be the adjoint representation of
. The trace field of
is the field:
k\Gamma=Q(\{\operatorname{trace}(\rho(\gamma)):\gamma\in\Gamma\}).
If two Zariski-dense subgroups of
are commensurable then they have the same trace field in this sense.
The trace field for lattices
Let
be a semisimple Lie group and
a
lattice. Suppose further that either
is irreducible and
is not locally isomorphic to
, or that
has no factor locally isomorphic to
. Then
local rigidity implies the following result.
The field
is a
number field.
over
such that the group of real points
is isomorphic to
and
is contained in a conjugate of
. Thus
is a "field of definition" for
in the sense that it is a
field of definition of its
Zariski closure in the adjoint representation.
In the case where
is
arithmetic then it is commensurable to the arithmetic group defined by
.
For Fuchsian groups the field defined above is equal to its invariant trace field. For Kleinian groups they are the same if we use the adjoint representation over the complex numbers.
References
- News: Vinberg . Ernest . Rings of definition of dense subgroups of semisimple linear groups . Izv. Akad. Nauk SSSR Ser. Mat. . 35 . 1971 . 45–55 . 0279206 . Russian.
- Book: Maclachlan . Colin . Reid . Alan . The arithmetic of hyperbolic 3-manifolds . 2003 . Springer.
- Book: Margulis, Grigory . Discrete subgroups of semisimple Lie groups . . Ergebnisse de Mathematik und ihrer Grenzgebiete . 1991 . 3-540-12179-X . 1090825 .