### Abstract

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.

Original language | English |
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Pages (from-to) | 206-214 |

Number of pages | 9 |

Journal | JETP Letters |

Volume | 101 |

Issue number | 3 |

DOIs | |

Publication status | Published - 1 Feb 2015 |

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### ASJC Scopus subject areas

- Physics and Astronomy (miscellaneous)

### Cite this

**Properties of electrons scattered by a strong plane electromagnetic wave with a linear polarization : Semiclassical treatment.** / Bogdanov, O. V.; Kazinskii, Petr Olegovich.

Research output: Contribution to journal › Article

*JETP Letters*, vol. 101, no. 3, pp. 206-214. https://doi.org/10.1134/S0021364015030030, https://doi.org/10.1134/S0021364015030030

}

TY - JOUR

T1 - Properties of electrons scattered by a strong plane electromagnetic wave with a linear polarization

T2 - Semiclassical treatment

AU - Bogdanov, O. V.

AU - Kazinskii, Petr Olegovich

PY - 2015/2/1

Y1 - 2015/2/1

N2 - 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.

AB - 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.

UR - http://www.scopus.com/inward/record.url?scp=84928692532&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=84928692532&partnerID=8YFLogxK

U2 - 10.1134/S0021364015030030

DO - 10.1134/S0021364015030030

M3 - Article

AN - SCOPUS:84928692532

VL - 101

SP - 206

EP - 214

JO - JETP Letters

JF - JETP Letters

SN - 0021-3640

IS - 3

ER -