“…The other check that needs to be made is that for stable weights λ ∈ P + (q n ), µ ∈ P + (q n ), and for t ∈ C, we have However following the argument of Lemma 6.5.4, we see that the main step is to take an eigenspace of a certain semisimple operator z, which clearly commutes with h since they both lie in t. Thus Lemma 6.5.4 becomes, in our case, [DS x (L(λ)) : L gx (ν) t ] = [DS x (L g ′ ×h ′′ (λ)) : L g ′ x ×h ′′ (ν) t ]. Now using the statement of Lemma 6.5.5 along with this, we obtain Equation (15).…”