Abstract
The mathematical model for a racetrack microtron with an output energy of 50 MeV is described. The number of orbits is five. The increment of energy beam increase is 10 MeV per turn. The frequency rate of acceleration is four. One feature of the accelerator is injection directly into the acceleration section with a rather low kinetic energy beam of 0.8–1 MeV. The parameters that affect the capture region in the acceleration mode are determined. The region of capture is calculated. The basic properties of the focusing system are studied. The conditions for the optimum passage of the beam are substantiated for all orbits.
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