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Radiation from a beam of modulated electrons. II
1.H. Schwarz and H. Hora, Appl. Phys. Letters 15, 349 (1969).
2.C. Becchi and G. Morpurgo, Phys. Rev. D 4, 288 (1971).
3.This information was also directly communicated to Dr. H. Schwarz by the authors.
4.At least three but more realistically five orders of magnitude.
5.H. Schwarz, Proceedings of the Second International Conference on Light Scattering in Solids, edited by M. Balkanski (Flammarion, Paris, 1971), p. 123.
6.L. L. Van Zandt, Appl. Phys. Letters 17, 345 (1970).
7.Summing Eq. (1) over all the final states, one gets the structure of formula (7) of Van Zandt (Ref. 2) is instead, in the present notation, which is of course different. The reason for the difference lies in the fact that Van Zandt has treated the electric field due to an electron as a c number instead of as an operator.
8.Phys. Today 24, 17 (1971).
8.Compare also the recent answer by H. Schwarz [Appl. Phys. Letters 20, 148 (1972)]
8.to the remarks on the intensity of the electron beam contained in a letter by L. Pfeiffer, D. Rousseau, and A. R. Hutson, Appl. Phys. Letters 20, 147 (1972).
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