Laser-driven relativistic tunneling from p-states
arXiv:1410.3324 · doi:10.1103/PhysRevA.90.063416
Abstract
The tunneling ionization of an electron from a p-state in a highly charged ion in the relativistic regime is investigated in a linearly polarized strong laser field. In contrast to the case of an s-state, the tunneling ionization from the p-state is spin asymmetric. We have singled out two reasons for the spin asymmetry: first, the difference of the electron energy Zeeman splitting in the bound state and during tunneling, and second, the relativistic momentum shift along the laser propagation direction during the under-the barrier motion. Due to the latter, those states are predominantly ionized where the electron rotation is opposite to the electron relativistic shift during the under-the-barrier motion. We have investigated the dependence of the ionization rate on the laser intensity for different projections of the total angular momentum and identified the intensity parameter which governs this behaviour. The significant change of the ionization rate is originated from the different precession dynamics of the total angular momentum in the bound state at high and low intensities.
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Cited by in corpus (8)
- Theory of Radiative Electron Polarization in Strong Laser Fields
- Spin-polarizing interferometric beam splitter for free electrons
- Supercontinuum in ionization by relativistically intense and short laser pulses: ionization without interference and its time analysis
- Above-threshold ionization with highly charged ions in super-strong laser fields: III. Spin effects and its dependence on laser polarization
- Electron spin filter and polarizer in a standing light wave
- Spin in Compton scattering with pronounced polarization dynamics
- Scaling relations of the time-dependent Dirac equation describing multiphoton ionization of hydrogen-like ions
- Generation of attosecond electron beams in relativistic ionization by short laser pulses