“…In a first step one neglects the Weyl symmetry to simplify the matter. For this purpose one defines the operator δ as 34) or in terms of the basic fields δη a = −e a , δφ = 0 for φ = (ϕ, ω, e, R, T, θ) . It is easy to verify that δ is of degree zero and that, together with the BRST operator s, it obeys the following algebraic relations: One sees from eq.…”