On hypersymmetry in three dimensions

Abstract

In this work we presented a number of explicit examples for the cubic vertices describing an interaction of massless spin- frac{5}{2} field with massive boson and fermion including all hypertransformations necessary for the vertices to be gauge invariant. Here we restrict ourselves with the massive bosons with spins s = 2, 1, 0 and massive fermions with spins s = frac{3}{3} , frac{1}{2} . Our general analysis predicted that the vertex must exist for any boson and fermion with the spin difference frac{3}{2} or frac{1}{2} . And indeed it appeared that the vertex exists for all six possible pairs (2, 1, 0) ⊗ ( frac{3}{2} , frac{1}{2} ). As in the case of massive supermultiplets, our construction is based on the gauge invariant description for the massive fields with spins s ≥ 1. Moreover, we have explicitly checked that all the vertices are invariant also under the gauge symmetries of these massive fields.