Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Reference8 articles.
1. B. De Tollis:Nuovo Cimento,32, 757 (1964) (henceforth referred to as A). Further references are given in A. We want to point out two misprints in that paper: 1) p. 759, line 10: for « … interchanges 2 ↔ 3 and 3 ↔ 4 » read « … interchanges 2 ↔ 4 and 3 ↔ 4 »; 2) p. 768, eq. (II.4): the lower limit of the integration is 1 instead of 0.
2. R. Karplus andM. Neuman:Phys. Rev.,83, 776 (1951). In this paper, it seems to us that the expressions for the amplitudesM ++++ andM ++−− have been interchanged, for a misprint, in eqs. (23) (low-energy limit) and in Table II (right-angle scattering).
3. These weight factors are in accord also with those given by KN in eq. (7) of their paper. The weights of the linear polarization states, when they are summed up, give 8 instead of 16, as in the case of circular polarizations. In fact, for linear polarizations the not vanishing amplitudes are only 8.Jauch andRohrlich, perhaps, do not bear in mind this circumstance when they suggest that the weights of the linear polarization states, as given by KN, must be multiplied by a factor of two (J. M. Jauch andF. Rohrlich:The Theory of Photons and Electrons, (Cambridge, 1955), p. 294, footnote).
4. For the Spence (or dilogarithm) function which appears in the functionI see for example:K. Mitchell:Phil. Mag.,40, 351 (1949).
5. G. Breit andJ. A. Wheeler:Phys. Rev.,46, 1087 (1934).
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