“…However, in order to apply bosonization one has to restrict the elements g ∈ N G (h) ⊂ G to the Cartan normalizer, and this will be the key object in our definition of the twist fields. In particular, bosonization means that one considers the space H˙g as a sum of twisted representations of the Heisenberg algebra h. These representations depend not only on the elements g ∈ N G (h), but also on additional data: eigenvalues of the zero modes of the ginvariant part of h. This extra data, below to be called r-charges following [16], has discrete freedom, since only the exponents of such eigenvalues are specified by g. We also denote below the most refined data asg = (g, r).…”