Let be a Lie group. We are interested in the infinite dimensional Lie group
where composition is done pointwise. One way to understand a group is by understanding its representations. In this particular case our interest is quickly narrowed to smooth, projective, positive energy representations. It turns out that a better way object of study is the semidirect product
where
is a particular one dimensional central extension and
acts on
by rotating loops (that is precomposing
with a rotation).
This thing’s Lie Algebra will be (as a vectors space) . My charge, by this Sunday, is to calculate the Lie bracket. Suffice we will consider the (dense?) subalgebra
To begin with:
because rotation is commutative. The centeral extension is, well, central so we have:
What’s left are
Lets start with the first. We’ll take what I’ll call the “scenic route” doing as much explicit calculation as possible.
| where and |
e.g. |
The second calculation is actually fixed for us by the particular type of central extension we’re using. I’ll explain tomorrow.
June 24, 2008 at 4:03 pm |
oops…”tomorrow” has turned into “next week”