Let (M,g) be a spin manifold with spinorial connection ∇. The Seiberg-Witten equations for spinorial connection are:
∇Yψ=−ig(Y,X)ψ
dX∗+=i<(YZ−ZY).ψ,ψ>
With ψ a spinor and X a vector field, Y,Z are variable vector fields.
The gauge group is f:M→S1, it acts on the solutions:
f.(X,ψ)=(X+idf∗f,fψ)
The moduli space is the quotient by the action of the gauge group.
Can we make Seiberg-Witten theory for spinorial connection?