Physical interpretation
The BRST-nontrivial deformations of the action are called integrated vertices
because they are integrals over the worldsheet of a dimension-(1,1) operator:
We interpret Eq. (7) as a requirement that the OPE of the integrated
vertex operator with the -ghost be BRST-exact up to a total derivative.
It was pointed out by Nelson that
and
could be non-zero. Only their difference (denoted ) should be zero.
This is because, in order to define the integration over the moduli space, we do not
actually need the integration form to be completely horizonthal.
There is some partial canonical gauge fixing.