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arXiv · 0910.4268

Radiation back-reaction in relativistically strong and QED-strong laser fields

Igor V. Sokolov·John A. Nees·Victor P. Yanovsky·Natalia M. Naumova·Gerard A. Mourou
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Abstract

The emission from an electron in the field of a relativistically strong laser pulse is analyzed. At the pulse intensities of \ge 10^{22} W/cm^2 the emission from counter-propagating electrons is modified by the effects of Quantum ElectroDynamics (QED), as long as the electron energy is sufficiently high: E \ge 1 GeV. The radiation force experienced by an electron is for the first time derived from the QED principles and its applicability range is extended towards the QED-strong fields.

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Igor V. Sokolov, John A. Nees, Victor P. Yanovsky, Natalia M. Naumova, Gerard A. Mourou. 2009-10-22. Radiation back-reaction in relativistically strong and QED-strong laser fields. https://doi.org/10.1063/1.3426068

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