Using the quantitative rescattering model, we simulate the correlated two-electron momentum distributions for nonsequential double ionization of helium by 800 nm laser pulses at intensities in the range of (2 − 15) × 1014W/cm2. The experimentally observed V-shaped structure at high intensities [Phys. Rev. Lett.99,263003(2007)10.1103/PhysRevLett.99.263003] is attributed to the strong forward scattering in laser-induced recollision excitation and the asymmetric momentum distribution of electrons that are tunneling-ionized from the excited states. The final-state electron repulsion also plays an important role in forming the V-shaped structure.
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The Role of Polarization for Bound States in Strong Fields
Abstract As atomic matter interacts with ultrastrong fields, the bound electrons are polarized and have ionization energies changed by Stark-shifting. The unprecedented range of laser intensities from 1015W cm−2to 1024W cm−2can take the interaction from the neutral atom to a bare nucleus. We have used an outer, single active electron approximation to calculate the polarization and Stark-shifted binding energy for ultraintense lasers interacting with highly charged ions at intensities from 1014W cm−2to 1022W cm−2. The polarization of the bound state can result in a dipole moment and Stark shift that may be 0.1 e a0and 50 Eh, respectively. At these high intensities, relativistic effects must also be considered. Across the intensity range of these studies, the magnetic field of the laser does not comparably affect the bound state of the atom; the impact of polarization and Stark shift exceed changes to the bound state wave function and binding energy from including relativity.
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- Award ID(s):
- 2110462
- PAR ID:
- 10647026
- Publisher / Repository:
- IOP Publishing
- Date Published:
- Journal Name:
- Journal of Physics: Conference Series
- Volume:
- 2894
- Issue:
- 1
- ISSN:
- 1742-6588
- Page Range / eLocation ID:
- 012007
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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