corner
corner

Phys. Rev. A 80, 023426 (2009) [8 pages]

Attosecond photoelectron microscopy of H2+

Download: PDF (313 kB) Buy this article Export: BibTeX or EndNote (RIS)

S. X. Hu*
Laboratory for Laser Energetics, University of Rochester, 250 E. River Road, Rochester, New York 14623, USA

L. A. Collins
Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA

B. I. Schneider
Office of Cyberinfrastructure and Physics Division, National Science Foundation, Arlington, Virginia 22230, USA

Received 13 May 2009; published 31 August 2009

See accompanying Physics Viewpoint

We present a numerical study of the ultrafast ionization dynamics of H2+ exposed to attosecond extreme ultraviolet (xuv) pulses that goes beyond the Born-Openheimer approximation. The four-dimensional, time-dependent Schrödinger equation was solved using a generalization of the finite-element discrete-variable-representation/real-space–product technique used in our previous calculations to include the dynamical motion of the nuclei. This has enabled us to expose the target to any polarized light at arbitrary angles with respect to the molecular axis. Calculations have been performed at different angles and photon energies (ω=50 eV up to 630 eV) to investigate the energy and orientation dependence of the photoionization probability. A strong orientation dependence of the photoionization probability of H2+ was found at a photon energy of ω=50 eV. At this energy, we found that the ionization probability is three times larger in the perpendicular polarization than in the parallel case. These observations are explained by the different geometric “cross sections” seen by the photoejected electron as it leaves the molecule. This ionization anisotropy vanishes at the higher-photon energy of ω≥170 eV. When these higher-energy xuv pulses are polarized perpendicular to the internuclear axis, a “double-slit-like” interference pattern is observed. However, we find that the diffraction angle only approaches the classical formula ϕn=sin−1(nλe/R0), where n is the diffraction order, λe is the released electron wavelength, and R0 is the internuclear distance, when nλe becomes less than 65% of R0. These results illustrate the possibility of employing attosecond pulses to perform photoelectron microscopy of molecules.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.80.023426
DOI:
10.1103/PhysRevA.80.023426
PACS:
33.80.Rv, 32.80.Rm

*shu@lle.rochester.edu