With and the routing just described, multiplication of the three QED Feynman rules for the Feynman vertices, the two Dirac propagators and the photon propagator gives . Hence the unrenormalized amputated Feynman vertex through this order is
For the renormalized Feynman vertex, add to this expression. Contributions from replacing parameters inside the one-loop term by their bare counterparts enter at higher loop order.

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