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Reference4 articles.
1. See any treatise on quantum electrodynamics, and alsoT. A. Welton:Phys. Rev.,74, 1157 (1948). The physical meaning of the perturbative procedures was admirably illustrated byN. Bohr inAtomic Theory and the Description of Nature (The University Press, Cambridge, 1934; and AMS Press Inc., New York, N. Y., 1987),passim.
2. Cf., in particular,W. Heitler:The Quantum Theory of Radiation, third edition (Clarendon Press, Oxford, 1954), sect.16, 18, 33; andG. Källén:Quantenelektrodynamik, Bd. 5/1 of theHandbuch der Physik (Springer-Verlag, Berlin, etc., 1958), Ziff. 28.
3. P. Bocchieri, A. Crotti andA. Loinger:Lett. Nuovo Cimento,4, 741 (1972);P. Bocchieri, A. Loinger andF. Valz-Gris:Nuovo Cimento B,19, 1 (1974);G. Casati, I. Guarneri andF. Valz-Gris:Phys. Rev. A,16, 1237 (1977);G. Benettin andL. Galgani:J. Stat. Phys.,27, 153 (1982);G. Casati, I. Guarneri andF. Valz-Gris:J. Stat. Phys.,30, 195 (1983); and other papers.
4. A treatment of the nonrelativistic electron, based on a Heisenberg equation of motion analogous to our eq. (4), presents some unsolved difficulties, cf.G. M. Prosperi andA. Scotti:Nucl. Phys.,13, 140 (1959).
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