Inquantum electrodynamics, thevertex function describes the coupling between aphoton and anelectron beyond the leading order ofperturbation theory. In particular, it is theone particle irreducible correlation function involving thefermion, the antifermion, and thevector potentialA.
The vertex function can be defined in terms of afunctional derivative of theeffective action Seff as

The dominant (and classical) contribution to is thegamma matrix, which explains the choice of the letter. The vertex function is constrained by the symmetries of quantum electrodynamics —Lorentz invariance;gauge invariance or thetransversality of the photon, as expressed by theWard identity; and invariance underparity — to take the following form:
where, is the incoming four-momentum of the external photon (on the right-hand side of the figure), andF1(q2) andF2(q2) are the Dirac and Pauliform factors,[1] respectively, that depend only on the momentum transferq2. At tree level (or leading order),F1(q2) = 1 andF2(q2) = 0. Beyond leading order, the corrections toF1(0) are exactly canceled by thefield strength renormalization. The form factorF2(0) corresponds to theanomalous magnetic momenta of the fermion, defined in terms of theLandé g-factor as:
In 1948,Julian Schwinger calculated the first correction to anomalous magnetic moment, given by
whereα is thefine-structure constant.[2]
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