Self-absorption of synchrotron radiation in a laser-irradiated plasma
arXiv:2005.00302 · doi:10.1063/5.0044766
Abstract
Electrons at the surface of a plasma that is irradiated by a laser with intensity in excess of are accelerated so strongly that they emit bursts of synchrotron radiation. Although the combination of high photon and electron density and electromagnetic field strength at the plasma surface makes particle-particle interactions possible, these interactions are usually neglected in simulations of the high-intensity regime. Here we demonstrate an implementation of two such processes: photon absorption and stimulated emission. We show that, for plasmas that are opaque to the laser light, photon absorption would cause complete depletion of the multi-keV region of the synchrotron photon spectrum, unless compensated by stimulated emission. Our results motivate further study of the density dependence of QED phenomena in strong electromagnetic fields.
arXiv comment20 pages, 4 figures; accepted version
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Cited by in corpus (5)
- Advances in QED with intense background fields
- Polarized QED cascades
- Nonlinear photon trident versus double Compton scattering and resummation of one-step terms
- Self-absorption of synchrotron radiation in a laser-irradiated plasma
- Dominance of - electron-positron pair creation in a plasma driven by high-intensity lasers