Vertex function

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Template:Short description 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 ψ, the antifermion ψ¯, and the vector potential A.

Definition

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

Γμ=1eδ3Seffδψ¯δψδAμ
File:Vertex correction.svg
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 Γμ is the gamma matrix γμ, 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:

Γμ=γμF1(q2)+iσμνqν2mF2(q2)

where σμν=(i/2)[γμ,γν], qν is the incoming four-momentum of the external photon (on the right-hand side of the figure), and Template:Math and Template:Math are the Dirac and Pauli form factors,[1] respectively, that depend only on the momentum transfer q2. At tree level (or leading order), Template:Math and Template:Math. Beyond leading order, the corrections to Template:Math are exactly canceled by the field strength renormalization. The form factor Template:Math corresponds to the anomalous magnetic moment a of the fermion, defined in terms of the Landé g-factor as:

a=g22=F2(0)

In 1948, Julian Schwinger calculated the first correction to anomalous magnetic moment, given by

F2(0)α2π

where α is the fine-structure constant.[2]

See also

References

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External links

Template:QED


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