“…Seiberg, avoiding the technicalities of super Feynman rules, presented in [22] and [23] an alternative derivation. Since we are mostly interested in perturbative effects we will follow [21] and state the non renormalisation theorem as follows: All contributions to the Wilsonian effective action from loop diagrams are of the form A G = d 4 θd 4 x 1 ...d 4 x n G(x 1 , ..., x n , θ,θ), (2.1) and involve an integral over all of superspace. In particular, no contributions arise of the form A W = d 2 θd 4 x 1 ...d 4 x n W (x 1 , ..., x n , θ) + c.c., (2.2) where the integral is only over the chiral subspace of superspace.…”