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Vertex function

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.

Definition

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The vertex function can be defined in terms of a functional derivative of the effective action Seff as

The one-loop correction to the vertex function. This is the dominant contribution to the anomalous magnetic moment of the electron.

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,[1] 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.[2]

See also

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References

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  1. ^ Wong, Samuel S. M. (2024-11-12). Introductory Nuclear Physics. John Wiley & Sons. ISBN 978-3-527-41445-1.
  2. ^ Teubner, Thomas (2018). "The anomalous anomaly". Nature Physics. 14 (11): 1148–1148. doi:10.1038/s41567-018-0341-3. ISSN 1745-2481.
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