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Reference6 articles.
1. Cf. P. A. M. Dirac, Proc. Royal Soc. A 167 (1938) 148; F. Rohrlich,Classical charged particles (Addison-Wesley, Reading, Mass. 1965).
2. As an example of the complexity of calculations for a particle of finite size, seeJ. S. Nodvik, Annals of Physics 28 (1964) 225.
3. Cf.J. L Synge,Relativity: the Special Theory (North-Holland, Amsterdam, 1965, p. 383) where the notation is slightly different.
4. dΩ is the invariant element of 2-content on the null cone; cf.Synge, p. 429 orThe Relativistic Gas (North-Holland, Amsterdam, 1957) p. 9.
5. Modification of the energy tensor to avoid renormalisation has been proposed byE. Arnous, J. Madore andA. Papapetrou, Nuovo Cimento 53A (1968) 393.
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