Ejection Energy of Photoelectrons in Strong Field Ionization
arXiv:physics/9611023 · doi:10.1103/PhysRevA.55.2180
Abstract
We show that zero ejection energy of the photoelectrons is classically impossible for hydrogen-like ions, even when field ionization occurs adiabatically. To prove this we transform the basic equations to those describing two 2D anharmonic oscillators. The same method yields an alternative way to derive the anomalous critical field of hydrogen-like ions. The analytical results are confirmed and illustrated by numerical simulations. PACS Number: 32.80.Rm
7 pages, REVTeX, postscript file including the figures is available at http://www.physik.th-darmstadt.de/tqe/dieter/publist.html or via anonymous ftp from ftp://tqe.iap.physik.th-darmstadt.de/pub/dieter/publ_I_pra_pre.ps, accepted for publication in Phys. Rev. A
Cited by in corpus (5)
- Exact field ionization rates in the barrier suppression-regime from numerical TDSE calculations
- A two-dimensional, two-electron model atom in a laser pulse: exact treatment, single active electron-analysis, time-dependent density functional theory, classical calculations, and non-sequential ionization
- High-order harmonic generation from Rydberg atoms driven by plasmonic-enhanced laser fields
- Ionization-induced laser-driven QED cascade in noble gases
- Electron residual energy due to stochastic heating in field-ionized plasma