On the In teractions of Mesons with the Electromagnetic Field

Abstract
By means of the formalism of Duffin and Kemmer there is constructed for mesons interacting with the electromagnetic field a theory that is manifestly Lorentz invariant and also gauge invariant and invariant under charge conjugation. The transformation to an interaction representation is accomplished by a procedure necessarily somewhat more complicated than that used by Schwinger for the quantum electrodynamics of electrons. The longitudinal components of the electromagnetic field are eliminated in a covariant manner.

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