Achieving a quantitative understanding of carrier-envelope phase effects in the benchmark H$_2^+$ molecule

POSTER

Abstract

The implementation of carrier-envelope phase (CEP) control over H$_2^+$ provides an ideal opportunity for a detailed, benchmark comparison of theory and experiment. Given complete experimental inputs, theory should, in principle, be able to reproduce the measured observables quantitatively. Nevertheless, the agreement in Ref. [1] was less than satisfactory. To try to explain the discrepancies, we theoretically consider (i) a non-Gaussian laser spectrum and (ii) the contribution of $n \ge 2$ manifolds and ionization. These two effects will be shown to produce non-trivial changes in the observables. \\[4pt] [1] N. G. Kling {\it et al}, Phys. Rev. Lett. {\bf 111}, 163004 (2013).

*This work was supported by the Chemical Sciences, Geosciences, and Biosciences Division, Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy under Grant No. DE-FG02-86ER13491. The PULSAR laser was provided by Grant No. DE-FG02-09

Authors

  • Shuo Zeng

    • J. R. Macdonald Laboratory, Kansas State University, Manhattan, Kansas, 66506
    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS, USA
    • J. R. Macdonald Laboratory, Physics Dept., Kansas State University, Manhattan, KS, USA
  • Nora Kling

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Kelsie Betsch

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Mohammad Zohrabi

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Fatima Anis

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Utuq Ablikim

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Bethany Jochim

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Zhenhua Wang

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Matthias Kuebel

    • Max-Planck-Institut fur Quantenoptik, Garching, Germany
  • Matthias Kling

    • Max-Planck-Institut fur Quantenoptik, Garching, Germany
  • Kevin Carnes

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Brett Esry

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University
  • Itzik Ben-Itzhak

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University