Vertex function

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 $\psi$, the antifermion $\overline{\psi }$, and the vector potential A. But the use of a vertex function is not limited to QED.

Definition

The vertex function ${\mathrm{\Gamma }}^{\mu }$ can be defined in terms of a functional derivative of the effective action S_eff as

${\mathrm{\Gamma }}^{\mu }=-\frac{1}{e}\frac{{\delta }^3{S}_{\mathrm{e}\mathrm{f}\mathrm{f}}}{\delta \overline{\psi }\delta \psi \delta A_{\mu }}$

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 ${\mathrm{\Gamma }}^{\mu }$ is the gamma matrix ${\gamma }^{\mu }$, 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:

${\mathrm{\Gamma }}^{\mu }={\gamma }^{\mu }{F}_1(q^2)+\frac{i{\sigma }^{\mu \nu }{q}_{\nu }}{2m}{F}_2(q^2)$

where ${\sigma }^{\mu \nu }=(i/2)[{\gamma }^{\mu },{\gamma }^{\nu }]$, $q_{\nu }$ 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, 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:

$a=\frac{g-2}{2}=F_2(0)$

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

$F_2(0)\approx \frac{\alpha }{2\pi }$

where α is the fine-structure constant.

See also

• Nonoblique correction

References

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External links

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