Abstract
The Dirac Maxwell equations are reformulated by eliminating that part of the interaction term which contributes only to the mass and charge of the bare electron and then by replacing the bare mass and charge of the electron by its experimental mass and charge. Then it is shown that a renormalization scheme is contained within them. Two schemes for renormalization are described and it is shown that the first scheme, although not the same, follows the pattern of Dyson’s renormalization program.
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