Abstract
The electromagnetic radiation generated by relativistic electrons undergoing centripetal acceleration is a subject which has received theoretical attention long before synchrotron radiation was even observed. Lienard1 obtained the first expression for the instantaneous power radiated by a relativistic charged particle. However, it was only during the 40’s that the classical theory of radiation losses in high energy circular accelerators was established almost simultaneously in the United States by Schwinger 2 and in the Soviet Union by Ivanenko, Pomeranchuk and Sokolov 3,4. Later on, the quantum theory corrections were examined and found to be important only when the momentum of the radiated photon is comparable with that of the electron, i.e. for very high electron energies of the order of 104 GeV 5,6.
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Wuilleumier, F.J. (1981). Atomic Physics with Synchrotron Radiation : Past, Present and Future. In: Kleppner, D., Pipkin, F.M. (eds) Atomic Physics 7. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-9206-8_21
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