Novel Aspects of Direct Laser Acceleration of Relativistic Electrons
arXiv:1502.06790 · doi:10.1017/S0022377815000434
Abstract
We examine the impact of several factors on electron acceleration by a laser pulse and the resulting electron energy gain. Specifically, we consider the role played by: 1) static longitudinal electric field; 2) static transverse electric field; 3) electron injection into the laser pulse; and 4) static longitudinal magnetic field. It is shown that all of these factors lead, under certain conditions, to a considerable electron energy gain from the laser pulse. In contrast with other mechanisms such as wakefield acceleration, the static electric fields in this case do not directly transfer substantial energy to the electron. Instead, they reduce the longitudinal dephasing between the electron and the laser beam, which then allows the electron to gain extra energy from the beam. The mechanisms discussed here are relevant to experiments with under-dense gas jets, as well as to experiments with solid-density targets involving an extended pre-plasma.
References in corpus (1)
Cited by in corpus (12)
- Enhanced proton acceleration in an applied longitudinal magnetic field
- Extremely intense laser-based electron acceleration in a plasma channel
- Scaling laws for direct laser acceleration in a radiation-reaction dominated regime
- Vacuum laser acceleration of super-ponderomotive electrons using relativistic transparency injection
- Impact of ion dynamics on laser-driven electron acceleration and gamma-ray emission in structured targets at ultra-high laser intensities
- Broadening of Cyclotron Resonance Conditions in the Relativistic Interaction of an Intense Laser with Overdense Plasmas
- Particle Deceleration for Collective QED Signatures
- Accurate simulation of direct laser acceleration in a laser wakefield accelerator
- Progress in relativistic laser-plasma interaction with kilotesla-level applied magnetic fields
- Generation of focusing ion beams by magnetized electron sheath acceleration
- Ambient air plasma acceleration in tightly-focused ultrashort infrared laser beams
- Emission of electromagnetic waves as a stopping mechanism for nonlinear collisionless ionization waves in a high- regime