Ghost number 1The elements ofcorrespond to the global symmetry currents of the
-model. There are finitely many global symmetries. We have:
We will now show thatis a finite-dimensional representation of
, actually the adjoint representation of
. How do we see this?
As a representation of,
is generated by the following objects:
Remember
are defined from
and similarly
.
The bar over indexmeans:
We see that
is a finite-dimensional space.
Why there are no more elements? For example, let us consider
. Modulo
this is same as
, and using Eq. (39) this is proportional to
.
Similarly, all the other covariant derivatives of every element of (50) can be expressed as a linear sum of other elements. Therefore, they form a closed representation of
.