Synchronous motion of a relativistic particle in a wave propagating at an angle to a magnetic field

It is shown that there is a special regime of motion of a relativistic particle in a transverse or longitudinal wave propagating at an angle to a magnetic field, which is called synchronous and in which the condition for resonance of the particle with the wave is satisfied with increasing accuracy as the particle energy increases. In the synchronous regime of Cherenkov resonance a trend to unbounded acceleration is observed. © 1996 American Institute of Physics.

Авторы
Журнал
Издательство
American Institute of Physics Inc.
Номер выпуска
5
Язык
Английский
Страницы
478-482
Статус
Опубликовано
Том
41
Год
1996
Организации
  • 1 Russian University of Friendship among Peoples, 117198 Moscow, Russian Federation
Дата создания
19.10.2018
Дата изменения
10.03.2021
Постоянная ссылка
https://repository.rudn.ru/ru/records/article/record/821/