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  1. W. E. Lamb. Jr., Phys. Rev. 85, 259 (1952), Secs. 51 and 54(d). See also S. J. Brodsky and R. G. Parsons, ibid. 163. 134 (1967).
  2. A lucid plausibility argument is given by H. A. Bethe and E. D. Salpeter, in Encyclopedia of Physics Vol. 35, S. Flügge, Ed., (Springer-Verlag, Berlin, 1957), Sec. 47β.
  3. This simple conservation law must have been noticed by many; I first heard it from E. C. Lerner. An obvious analog holds when the two charges are not equal and opposite.
  4. For a situation witlh some parallels, see E. Breitenberger, Am. J. Phys. 36. 504 (1968).
  5. Recent references: H. H. Denman, J. Math. Phys. 6, 1611 (1965) and 7, 1910 (1966); C. A. López, Nuovo Cimento 40, 19 (1965); B. Podolsky, Am. J. Phys. 34, 42 (1966).
  6. Physically, this term corresponds to an electrodynamic Stark effect [W. Wien, Ann. Physik 49, 842 (1916)] caused by the joint motion of the two charges across the magnetic-field lines (cf. also Lamb, Ref. 1); it has the requisite form -e(-E.r) for a constant, homogeneous electric field E = (P/M) × B.
  7. V. Berestetsky, Zh. Eksperim. i Teor. Fiz. 19, 1130 (1949) (in Russian). Also Bethe and Salpeter, Ref. 2, Sec. 23.
  8. L. I. Schiff and H. Snyder, Phys. Rev. 55, 59 (1939); D. Harting and P. F. A. Klinkenberg, Physica 14, 669 (1949); and further references given therein.

Berestetsky, V.

V. Berestetsky, Zh. Eksperim. i Teor. Fiz. 19, 1130 (1949) (in Russian). Also Bethe and Salpeter, Ref. 2, Sec. 23.

Betlhe, H. A.

A lucid plausibility argument is given by H. A. Bethe and E. D. Salpeter, in Encyclopedia of Physics Vol. 35, S. Flügge, Ed., (Springer-Verlag, Berlin, 1957), Sec. 47β.

Breitenberger, E.

For a situation witlh some parallels, see E. Breitenberger, Am. J. Phys. 36. 504 (1968).

Denman, H. H.

Recent references: H. H. Denman, J. Math. Phys. 6, 1611 (1965) and 7, 1910 (1966); C. A. López, Nuovo Cimento 40, 19 (1965); B. Podolsky, Am. J. Phys. 34, 42 (1966).

Lamb, Jr., W. E.

W. E. Lamb. Jr., Phys. Rev. 85, 259 (1952), Secs. 51 and 54(d). See also S. J. Brodsky and R. G. Parsons, ibid. 163. 134 (1967).

Salpeter, E. D.

A lucid plausibility argument is given by H. A. Bethe and E. D. Salpeter, in Encyclopedia of Physics Vol. 35, S. Flügge, Ed., (Springer-Verlag, Berlin, 1957), Sec. 47β.

Schiff, L. I.

L. I. Schiff and H. Snyder, Phys. Rev. 55, 59 (1939); D. Harting and P. F. A. Klinkenberg, Physica 14, 669 (1949); and further references given therein.

Snyder, H.

L. I. Schiff and H. Snyder, Phys. Rev. 55, 59 (1939); D. Harting and P. F. A. Klinkenberg, Physica 14, 669 (1949); and further references given therein.

Other (8)

W. E. Lamb. Jr., Phys. Rev. 85, 259 (1952), Secs. 51 and 54(d). See also S. J. Brodsky and R. G. Parsons, ibid. 163. 134 (1967).

A lucid plausibility argument is given by H. A. Bethe and E. D. Salpeter, in Encyclopedia of Physics Vol. 35, S. Flügge, Ed., (Springer-Verlag, Berlin, 1957), Sec. 47β.

This simple conservation law must have been noticed by many; I first heard it from E. C. Lerner. An obvious analog holds when the two charges are not equal and opposite.

For a situation witlh some parallels, see E. Breitenberger, Am. J. Phys. 36. 504 (1968).

Recent references: H. H. Denman, J. Math. Phys. 6, 1611 (1965) and 7, 1910 (1966); C. A. López, Nuovo Cimento 40, 19 (1965); B. Podolsky, Am. J. Phys. 34, 42 (1966).

Physically, this term corresponds to an electrodynamic Stark effect [W. Wien, Ann. Physik 49, 842 (1916)] caused by the joint motion of the two charges across the magnetic-field lines (cf. also Lamb, Ref. 1); it has the requisite form -e(-E.r) for a constant, homogeneous electric field E = (P/M) × B.

V. Berestetsky, Zh. Eksperim. i Teor. Fiz. 19, 1130 (1949) (in Russian). Also Bethe and Salpeter, Ref. 2, Sec. 23.

L. I. Schiff and H. Snyder, Phys. Rev. 55, 59 (1939); D. Harting and P. F. A. Klinkenberg, Physica 14, 669 (1949); and further references given therein.

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