4.2 Article

Intensity dependence of the attosecond control of the dissociative ionization of D2

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0953-4075/47/12/124020

Keywords

carrier-envelope phase; strong-field physics; electron dynamics; molecular dynamics

Funding

  1. Max Planck Society
  2. DFG [K1-1439/5]
  3. Cluster of Excellence: Munich Center for Advanced Photonics (MAP)
  4. American University of Sharjah
  5. Japan Society for the Promotion of Science [C24540421]
  6. HA-PACS Project for advanced interdisciplinary computational sciences by exa-scale computing technology
  7. King Saud University
  8. Arab Fund for Economic and Social Development (State of Kuwait)
  9. Grants-in-Aid for Scientific Research [24540421] Funding Source: KAKEN

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Light-field driven electron localization in deuterium molecules in intense near single-cycle laser fields is studied as a function of the laser intensity. The emission of D+ ions from the dissociative ionization of D-2 is interrogated with single-shot carrier-envelope phase (CEP)-tagged velocity map imaging. We explore the reaction for an intensity range of (1.0-2.8) x 10(14) W cm(-2), where laser-driven electron recollision leads to the population of excited states of D-2(+). Within this range we find the onset of dissociation from 3 sigma states of D-2(+) by comparing the experimental data to quantum dynamical simulations including the first eight states of D-2(+). We find that dissociation from the 3 sigma states yields D+ ions with kinetic energies above 8 eV. Electron localization in the dissociating molecule is identified through an asymmetry in the emission of D+ ions with respect to the laser polarization axis. The observed CEP-dependent asymmetry indicates two mechanisms for the population of 3 sigma states: (1) excitation by electron recollision to the lower excited states, followed by laser-field excitation to the 3 sigma states, dominating at low intensities, and (2) direct excitation to the 3 sigma states by electron recollision, playing a role at higher intensities.

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