Properties of electrons scattered by a strong plane electromagnetic wave with a linear polarization: semiclassical treatment

The problem of scattering of ultrarelativistic electrons by a strong plane electromagnetic wave of a low (optical) frequency and linear polarization is solved in the semiclassical approximation, when the electron wave packet size is much smaller than the wavelength of electromagnetic wave. The exit...

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Bibliographic Details
Published in:Journal of experimental and theoretical physics letters Vol. 101, № 3. P. 206-214
Main Author: Bogdanov, O. V.
Corporate Authors: Томский государственный университет Физический факультет Научные подразделения ФФ, Томский государственный университет Физический факультет Кафедра квантовой теории поля
Other Authors: Kazinski, P. O.
Format: Article
Language:English
Subjects:
Online Access:http://vital.lib.tsu.ru/vital/access/manager/Repository/vtls:000532439
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520 3 |a The problem of scattering of ultrarelativistic electrons by a strong plane electromagnetic wave of a low (optical) frequency and linear polarization is solved in the semiclassical approximation, when the electron wave packet size is much smaller than the wavelength of electromagnetic wave. The exit momenta of ultrarelativistic electrons scattered are found using the exact solutions to the equations of motion with radiation reaction included (the Landau-Lifshitz equation). It is found that the momentum components of electrons traversed the electromagnetic wave depend weakly on the initial values of momenta. These electrons are mostly scattered at small angles to the propagation direction of the electromagnetic wave. The maximum Lorentz factor of electrons crossed the electromagnetic wave is proportional to the work done by the electromagnetic field and is independent of the initial momentum. The momentum component parallel to the electric field vector of the electromagnetic wave is determined solely by the laser beam diameter measured in the units of the classical electron radius. As for the reflected electrons, they for the most part lose the energy, but remain relativistic. A reflection law that relates the incident and reflection angles and is independent of any parameters is found. 
653 |a электромагнитные волны 
653 |a Ландау-Лифшица уравнение 
653 |a линейная поляризация 
655 4 |a статьи в журналах  |9 879358 
700 1 |a Kazinski, P. O.  |9 385647 
710 2 |a Томский государственный университет  |b Физический факультет  |b Научные подразделения ФФ  |9 107954 
710 2 |a Томский государственный университет  |b Физический факультет  |b Кафедра квантовой теории поля  |9 77220 
773 0 |t Journal of experimental and theoretical physics letters  |d 2015  |g Vol. 101, № 3. P. 206-214  |x 0021-3640 
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