Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au
Last update: 22 December 2013
Affine Braid Group Representations and the Functors
There are three common ways of depicting affine braids [Cri1997], [GLa1997], [Jon1994]:
(a)
As braids in a (slightly thickened) cylinder,
(b)
As braids in a (slightly thickened) annulus,
(c)
As braids with a flagpole.
See Figure 1. The multiplication is by placing one cylinder on top of an- other, placing one annulus inside another, or placing one flagpole braid on top of another.
These are equivalent formulations: an annulus can be made into a cylinder by turning up the edges, and a cylindrical braid can be made into a flagpole braid
by putting a flagpole down the middle of the cylinder and pushing the pole over to the left so that the strings begin and end to its right.
The affine braid group is the group formed by the affine braids with
strands. The affine braid group can be presented by generators
and
with relations
Define
By drawing pictures of the corresponding affine braids it is easy to check that the
all commute with each other and so
is an abelian subgroup of Let
be the free abelian group generated by
Then
where
for
The Module
Let be the Drinfeld-Jimbo quantum group associated to a finite dimensional complex
semisimple Lie algebra Let be a
in the category and let be a finite dimensional
module. Define
and in by
The following proposition is well known (see [Suz2000, Prop. B.2], [LRa1977, Prop. 2.19], or [Res1990]).
The map defined by
makes into a right module.
Proof.
It is necessary to show that
(a)
if
(b)
(c)
(d)
The relations (a) and (b) follow immediately from the definitions of and
and (c) is a particular case of the braid relation (2.12). The relation (d) is also a
consequence of the braid relation:
or equivalently,
A module is calibrated if the abelian group
defined in (3.4) acts semisimply on i.e. if has a basis of
simultaneous eigenvectors for the action of
If and are finite dimensional
modules then the module
defined in Proposition 3.1 is calibrated.
Proof.
Let be the set of dominant integral weights. Since and
are finite dimensional the
is semisimple for every
and
where and
Given a basis of
which respects the decomposition
one can construct a basis of which
respects the decomposition
Since
this new basis respects the decomposition
This procedure produces, inductively, a basis of
which respects the decompositions
for all The central element
in
acts on
by the constant
From (2.10), (2.11) and (2.14) it follows that acts on
by
where
is the projection onto
Thus acts diagonally on the basis
Define an anti-involution on by
for and
A contravariant form on a module is a symmetric
bilinear form
such that
Suppose is a in the category
and is a finite dimensional module. Let
and
be
forms on and
respectively. By (2.16),
for and
for
Thus it follows that the form
on
given by
for
is a
contravariant form on the
module
The Functor
Fix a finite dimensional module and an integrally dominant weight
in Let
be the category of finite dimensional modules and define a functor
Since an element of
is determined by the image of a generating highest weight vector of
the space can be identified with the vector space
of highest weight vectors of weight in
If is integrally dominant the highest possible weight of
is
Thus, viewing
as the space of highest weight vectors of weight in
where we use the notation
where the are the Chevalley generators of
In the case of the notation
is self explanatory—the notation in (3.7) is simply a way to define the same object for the quantum group
The functor is the composition of two functors: the functor
and the functor
The first is exact since is finite dimensional and the second is exact because when
is integrally dominant is projective, see
[Jan1980, p. 72]. Thus
Notes and references
This is a typed version of the paper Affine Braids, Markov Traces and the Category by Rosa Orellana and Arun Ram*.
*Research supported in part by National Science Foundation grant DMS-9971099, the National Security Agency and EPSRC grant GR K99015.
This paper is a slightly revised version of a preprint of 2001. We thank F. Goodman, A. Henderson and an anonymous referee for their very helpful comments on the original preprint.