Vertex function
Effective particle coupling beyond tree level
In quantum electrodynamics, the vertex function describes the coupling between a photon and an electron beyond the leading order of perturbation theory. In particular, it is the one particle irreducible correlation function involving the fermion , the antifermion
, and the vector potential A. But the use of a vertex function is not limited to QED.
01Definition
The vertex function can be defined in terms of a functional derivative of the effective action Seff as
The dominant (and classical) contribution to is the gamma matrix
, which explains the choice of the letter. The vertex function is constrained by the symmetries of quantum electrodynamics, Lorentz invariance; gauge invariance or the transversality of the photon, as expressed by the Ward identity; and invariance under parity, to take the following form:
where ,
is the incoming four-momentum of the external photon (on the right-hand side of the figure), and F1(q2) and F2(q2) are the Dirac and Pauli form factors, respectively, that depend only on the momentum transfer q2. At tree level (or leading order), F1(q2) = 1 and F2(q2) = 0. Beyond leading order, the corrections to F1(0) are exactly canceled by the field strength renormalization. The form factor F2(0) corresponds to the anomalous magnetic moment a of the fermion, defined in terms of the Landé g-factor as:
In 1948, Julian Schwinger calculated the first correction to anomalous magnetic moment, given by
where α is the fine-structure constant.

Sources and credits
This article is adapted from the Wikipedia article “Vertex function”, written by its contributors and licensed under CC BY-SA 4.0. Fathomly has changed the layout, removed citation markers, navigation and maintenance notices, and adjusted punctuation. This adapted version is shared under the same license. For references, see the original article.
Images, from Wikimedia Commons:
- Vertex correction.svg by User:Harmaa, Public domain
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