Asymptotics of physical solutions to the Lorentz-Dirac equation for planar motion in constant electromagnetic fields / P. O. Kazinski, M. A. Shipulya

Уровень набора: Physical Review E, Scientific JournalОсновной Автор-лицо: Kazinski, P. O.Альтернативный автор-лицо: Shipulya, M. A., physicist, Associate Professor of Tomsk Polytechnic University, Candidate of Physical and Mathematical Sciences, 1986-, Mikhail AlekseevichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет, Физико-технический институт, Кафедра высшей математики и математической физикиЯзык: английский.Страна: .Резюме или реферат: We present a study of planar physical solutions to the Lorentz-Dirac equation in a constant electromagnetic field. In this case, we reduced the Lorentz-Dirac equation to one second-order differential equation. We obtained the asymptotics of physical solutions to this equation at large proper times. It turns out that, in a crossed constant uniform electromagnetic field with vanishing invariants, a charged particle enters a universal regime at large times. We found that the ratios of momentum components that tend to constants are determined only by the external field. This effect is essentially due to a radiation reaction. There is no such effect for the Lorentz equation in this field..Примечания о наличии в документе библиографии/указателя: [References: 39 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | уравнения | электромагнитное поле | асимптотика решений Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: 39 tit.]

We present a study of planar physical solutions to the Lorentz-Dirac equation in a constant electromagnetic field. In this case, we reduced the Lorentz-Dirac equation to one second-order differential equation. We obtained the asymptotics of physical solutions to this equation at large proper times. It turns out that, in a crossed constant uniform electromagnetic field with vanishing invariants, a charged particle enters a universal regime at large times. We found that the ratios of momentum components that tend to constants are determined only by the external field. This effect is essentially due to a radiation reaction. There is no such effect for the Lorentz equation in this field.

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