EPJ manuscript No. (will be inserted by the editor) Renormalization of QED in an external field Christian Brouder Laboratoire de Min´eralogie-Cristallographie, CNRS UMR7590, UPMC/UDD/IPGP, Case 115, 4 place Jussieu 75252 Paris cedex 05, France
[email protected] November 7, 2018 Abstract. The Schwinger equations of QED are rewritten in three different ways as integral equations involving functional derivatives, which are called weak field, strong field, and SCF quantum electrodynam- ics. The perturbative solutions of these equations are given in terms of appropriate Feynman diagrams. The Green function that is used as an electron propagator in each case is discussed in detail. The general renormalization rules for each of the three equations are provided both in a non perturbative way (Dyson relations) and for Feynman diagrams. PACS. 12.20.-m Quantum electrodynamics – 11.10.Gh Renormalization 1 Introduction The standard approach to QED comes clearly from particle physics, where the S matrix is most useful, and where in and out states of the scattering experiments This paper is a step towards the calculation of photon are well defined. In solid state physics, measurements are and electron spectroscopies of matter based on quantum usually based on a different principle. The spectroscopist electrodynamics. shines on the sample a beam of electrons or photons com- Starting from quantum electrodynamics, which is a ing from a classical source. By classical we mean that the most accurate and successful theory, garanties that the ba- source is not influenced by the system being measured. sis of the calculation is sound. Although such an approach After its interaction with the sample, another beam of may look too true to be beautiful, it seems adequate be- electrons or photons is measured.