Narrowing of the emission angle in high-intensity Compton scattering
arXiv:1507.06478 · doi:10.1103/PhysRevA.93.022112
Abstract
We consider the emission spectrum of high-energy electrons in an intense laser field. At high intensities () we find that the QED theory predicts a narrower angular spread of emissions than the classical theory. This is due to the classical theory overestimating the energy loss of the particles, resulting in them becoming more susceptible to reflection in the laser pulse.
7 pages, 6 figures
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- Unveiling the transverse formation length of nonlinear Compton scattering
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- WKB Electron Wave Functions in a Tightly Focused Laser Beam
- First-order strong-field QED processes including the damping of particles states
- In Situ Characterization of Ultraintense Laser Pulses
- One-photon pair-annihilation in pulsed plane-wave backgrounds
- Nonlinear Compton scattering and nonlinear Breit-Wheeler pair production including the damping of particle states
- The electron mass shift in an intense plane wave
- Scale invariance and scaling law of Thomson backscatter spectra by electron moving in laser-magnetic resonance regime
- Quasiclassical representation of the Volkov propagator and the tadpole diagram in a plane wave
- Optimized routines for event generators in QED-PIC codes
- Effect of electron-beam energy chirp on signatures of radiation reaction in laser-based experiments