Incoherent synchrotron emission of laser-driven plasma edge
arXiv:1508.05722 · doi:10.1063/1.4938206
Abstract
When a relativistically intense linearly polarized laser pulse is incident on an overdense plasma, a dense electron layer is formed on the plasma edge which relativistic motion results in high harmonic generation, ion acceleration and incoherent synchrotron emission of gamma-photons. Here we present a self-consistent analytical model that describes the edge motion and apply it to the problem of incoherent synchrotron emission by ultrarelativistic plasma electrons. The model takes into account both coherent radiation reaction from high harmonics and incoherent radiation reaction in the Landau-Lifshitz form. The analytical results are in agreement with 3D particle-in-cell simulations in a certain parameter region that corresponds to the relativistic electronic spring interaction regime.
References in corpus (5)
- All-optical Compton gamma-ray source
- Ultra-high brilliance multi-MeV -ray beam from non-linear Thomson scattering
- Enhanced relativistic harmonics by electron nanobunching
- The effect of non-linear quantum electrodynamics on relativistic transparency and laser absorption in ultra-relativistic plasmas
- Laser-driven hole boring and gamma-ray emission in high-density plasmas
Cited by in corpus (8)
- Theory of relativistic radiation reflection from plasmas
- Relativistically intense XUV radiation from laser-illuminated near-critical plasmas
- Near-surface electron acceleration during intense laser-solid interaction in the grazing incidence regime
- Weibel instability in hot plasma flows with production of gamma-rays and electron-positron pairs
- Controlling the ellipticity of attosecond pulses produced by laser irradiation of overdense plasmas
- Physics of the laser-plasma interface in the relativistic regime of interaction
- Piecewise acceleration of electrons across a periodic solid-state structure irradiated by intense laser pulse
- Employing machine learning for theory validation and identification of experimental conditions in laser-plasma physics