Begründung einer Integralgleichung für die Bewegung eines strahlenden Elektrons

Foundation of a Functional Equation of Motion for the Radiating Electron An integro-differential equation of motion for the radiating electron; proposed in an earlier paper, is founded on the Maxwell-Lorentz-theory. In 1^st order approximation and in the non-relativistic limit, our equation becomes identical with the theories of Herglotz (1903) and Kaup (1966).