Why is it that spin-32 fields are usually described to be in the (12,12)⊗[(12,0)⊕(0,12)] representation (Rarita-Schwinger) rather than the (32,0)⊕(0,32) representation? Does the latter not describe a spin-32 field? Why is the gravitino given by the Rarita-Schwinger-type representation rather than the (32,0)⊕(0,32) representation?
This is related to a recent question I asked on gauge invariance of the Rarita-Schwinger field.
Thanks!
No comments:
Post a Comment