Renormalizability of nonanticommutative N=(1,1)N=(1,1) theories with singlet deformation

We study the quantum properties of two theories with a nonanticommutative (or nilpotent) chiral singlet deformation of N=(1,1)N=(1,1) supersymmetry: the Abelian model of a vector gauge multiplet and the model of a gauge multiplet interacting with a neutral hypermultiplet. In spite of the presence of a negative-mass-dimension coupling constant (deformation parameter), both theories are shown to be finite in the sense that the full effective action is one-loop exact and contains finitely many divergent terms, which vanish on-shell. The β-function for the coupling constant is equal to zero. The divergencies can all be removed off shell by a redefinition of one of the two scalar fields of the gauge multiplet. These notable quantum properties are tightly related to the existence of a Seiberg–Witten-type transformation in both models.