Chirp control of the formation of excited neutral D fragments in intense ultrafast laser pulses

ORAL

Abstract

Excited neutral D fragments ($n$$\geq$2) are formed by the interaction of intense laser pulses with D$_2$ molecules [1]. One of the suggested interpretations of this process is that one (or both) of the electrons that were ejected recombine with the parent ion(s) and form the excited neutral fragment(s) [1]. In the present study, 400 nm laser pulses were used, and a single-prism pulse compressor [2] was implemented, which allows the generation of both positively- and negatively-chirped laser pulses. The kinetic energy release spectrum of neutral D fragments is observed to be extremely sensitive to the laser parameters. In particular, we report control of this spectrum using the chirp of the laser pulses. \\ {[1]} T. Nubbemeyer \emph{et al.}, Phys. Rev. Lett \textbf{101}, 233001 (2008). \\ {[2]} Selcuk Akturk \emph{et al.}, Opt. Express \textbf{14}, 10101 (2006).

*Supported by the Chemical Sciences, Geosciences, and Biosciences Division, Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy under Award \# DE-FG02-86ER13491.

Authors

  • Peyman Feizollah

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
  • Ben Berry

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
  • Travis Severt

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Physics Department, Kansas State University, Manhattan, KS 66506, USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
    • Department of Physics, Kansas State University, Manhattan KS, USA
    • J.R. Macdonald Laboratory, Kansas State University, Manhattan, KS 66506
  • Bethany Jochim

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
  • M. Zohrabi

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
  • Kanaka Raju Pandiri

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
    • Department of Physics, Kansas State University, Manhattan KS, USA
    • J.R. Macdonald Laboratory, Kansas State University, Manhattan, KS 66506
  • K. D. Carnes

    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
  • B. D. Esry

    • Kansas State University
    • J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, KS 66506 USA
    • J.R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan KS, USA
  • Itzik Ben-Itzhak

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