Let DRS be the Rarita-Schwinger operator and ˜ψ=∑aψa⊗ea with an orthonormal basis (ea) of vectors, ψa spinors and ∑aeaψa=0.
The Seiberg-Witten equations for spin 3/2 are:
DRSA˜ψ=0
F(A)+=ω(˜ψ)
with
ω(˜ψ)=∑a<(XY−YX).ψa,ψa>
It doesn't depend on the choice of the basis (ea).
Is the theory of Seiberg-Witten for the spin 3/2 commutativ?