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

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

2009-10-22

arxiv.org/abs/0910.4268v1

Physics

Plasma Physics

4 pages, 4 figures

Scientific paper

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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