Partial contributions of individual harmonics to the power of synchrotron radiation
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For synchrotron radiation, the partial contribution is defined as the ratio of the power radiated by an individual spectral harmonic, ν = 1, 2, 3 …, to the total (summed over ν) radiated power. A complete analysis of the dependence of the partial contribution on ν, polarization of the radiation, and energy of the particle is given.
KeywordsSynchrotron Radiation Radiation Power Linear Polarization Polarize Component Partial Contribution
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- 1.A. A. Sokolov and I. M. Ternov, eds., Synhrotron Radiation [in Russian], Nauka, Moscow (1996).Google Scholar
- 2.A. A. Sokolov and I. M. Ternov, Synhrotron Radiation, Akademic Verlag, Berlin; Pergamon Press, NY (1968).Google Scholar
- 3.V. A. Bordovitsyn, ed., Synhrotron Radiation Theory and Its Development, World Scientific, Singapore, New Jersey, London, Hong Kong (1999).Google Scholar
- 4.V. A. Bordovitsyn, ed., Theory of the Radiation of Relativistic Particles, Fizmatlit, Moscow (2002).Google Scholar
- 5.V. G. Bagrov, Opt. Spektrosk., 18, Issue 4, 541–544 (1965).Google Scholar
- 6.I. S. Gradshtein and I. M. Ryzhik, Tables of Integrals, Sums, Series, and Products [in Russian], Nauka, Moscow (1971).Google Scholar
- 7.V. G. Bagrov, G. F. Kopytov, G. K. Razina, and V. B. Tlyachev [in Russian], VINITI Dep. No. 7927-B85 of 12.11.1985.Google Scholar