Photoelectron Angular Distributions for Two-photon Ionization of Helium by Ultrashort Extreme Ultraviolet Free Electron Laser Pulses
arXiv:1204.4812 · doi:10.1088/0953-4075/46/16/164018
Abstract
Phase-shift differences and amplitude ratios of the outgoing and continuum wave packets generated by two-photon ionization of helium atoms are determined from the photoelectron angular distributions obtained using velocity map imaging. Helium atoms are ionized with ultrashort extreme-ultraviolet free-electron laser pulses with a photon energy of 20.3, 21.3, 23.0, and 24.3 eV, produced by the SPring-8 Compact SASE Source test accelerator. The measured values of the phase-shift differences are distinct from scattering phase-shift differences when the photon energy is tuned to an excited level or Rydberg manifold. The difference stems from the competition between resonant and non-resonant paths in two-photon ionization by ultrashort pulses. Since the competition can be controlled in principle by the pulse shape, the present results illustrate a new way to tailor the continuum wave packet.
5 pages, 1 table, 3 figures
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Cited by in corpus (8)
- Atomic, molecular and optical physics applications of longitudinally coherent and narrow bandwidth Free-Electron Lasers
- Maximum Elliptical Dichroism in Atomic Two-Photon Ionization
- Photoelectron distribution of non-resonant two-photon ionization of neutral atoms
- Breakdown of the electric dipole approximation at Cooper minima in direct two-photon ionisation
- Theoretical study of pulse delay effects in the photoelectron angular distribution of near-threshold EUV+IR two-photon ionization of atoms
- Photoelectron Angular Distributions of Nonresonant Two-Photon Atomic Ionization Near Nonlinear Cooper Minima
- Angle-resolved non-resonant two-photon single ionization of argon using 9.3 eV photons produced via high harmonic generation
- Relativistic effects in the non-resonant two-photon K-shell ionization of neutral atoms