For massless spinors case we can decompose momentum into Weyl sub-parts as
$$p = \lambda_{a}\tilde \lambda_{\dot a}.$$
But for the case of massive fermions can I do something like this? Decompose them into Weyl subparts with some additional terms? If so, how?
Why do I need it? I am performing a twistor transform for the equation of the process $q\bar q \to gg$ so I have to write the amplitude and the 4d delta function of the momentum and then Fourier transform the $\lambda$ and $\tilde \lambda$ separately.