I'm interested in a QFT model featuring a fermion derivative coupling like $XX^* \chi^*\gamma^\mu∂_\mu \psi$ where X is some other field operator. Has anybody seen a paper containing something like this? How would Feynman-Graphs for such an interaction look like? Are derivatives of fermions ruled out by some consideration i am missing?
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In four dimensions, the interaction term you have written is expected to render your field theory non-renormalizable. This is OK as far as modeling low energy physics is concerned. But, there is another problem. The interaction is not Hermitian (which would lead not non-unitary time evolution). Now, the Feynman rule that would be generated from this is a four-point interaction, involving the transformation of a spin-1/2 $\psi$ quanta into a $\chi$ quanta, with an associated emission of a $X$/$X*$ pair. The Feynman rule for such a vertex should be dependent on the momentum: $\text{vertex}=\gamma^\mu p_\mu$. |
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