The first-order Dyson series contains . For an amputated three-point Feynman diagram, each of the three distinct field types contracts in exactly one way. Writing each external plane wave in momentum space produces
Thus the momentum-space Feynman rule, with all four-momenta incoming, is
After stripping the conservation delta factor, it is simply . There is no combinatorial factor because the interaction has three distinct field slots. The charged lines carry opposite charge-flow orientations and the real heavy line is neutral.

Articles by others on the same topic (0)

There are currently no matching articles.