Strong-field control of H$_3^+$ formation pathways in methanol: Local versus extended H$_2$ roaming

POSTER

Abstract

Using the CD$_3$OH isotopologue of methanol, the ratio of D$_2$H$^+$ to D$_3^+$ formation is manipulated by changing the characteristics of the intense laser pulse. Formation of D$_2$H$^+$ indicates a process involving two hydrogen atoms from the methyl side of the target and a proton from the hydroxyl side, while detection of D$_3^+$ indicates direct formation involving only the methyl group. An adaptive control strategy that employs image-based feedback to guide the learning algorithm results in an enhancement of the D$_2$H$^+$/D$_3^+$ ratio by a factor of approximately two. The optimized pulses have time structures on the order of 100 fs. Systematic changes to the linear chirp and higher order dispersion terms of the laser pulse are compared to the results obtained with the optimized pulse shapes.

*Augustana University personnel and equipment were supported by National Science Foundation grant PHY-1723002. J.R. Macdonald Laboratory personnel and equipment were supported by the US Department of Energy under award \#DE-FG02-86ER13491.

Authors

  • Naoki Iwamoto

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • Charles J. Schwartz

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • J.L. Napierala

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • S.N. Tegegn

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • A. Solomon

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • S. Zhao

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • E. Wells

    • Department of Physics, Augustana University, Sioux Falls, SD 57197 USA
  • Bethany Jochim

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

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

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

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

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

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

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

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

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