Abstract
The emission from an electron in the field of a relativistically strong laser pulse is analyzed. At pulse intensities of J2× 1022W/ cm2 the emission from counterpropagating electrons is modified by the effects of quantum electrodynamics (QED), as long as the electron energy is sufficiently high: E1GeV. The radiation force experienced by an electron is for the first time derived from the QED principles and its applicability range is extended toward the QED-strong fields.
| Original language | English |
|---|---|
| Article number | 036412 |
| Journal | Physical Review E - Statistical, Nonlinear, and Soft Matter Physics |
| Volume | 81 |
| Issue number | 3 |
| DOIs | |
| Publication status | Published - 25 Mar 2010 |
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