- 1Department of Physics, Augustana University, Sioux Falls, SD, United States
- 2J. R. Macdonald Laboratory, Physics Department, Kansas State University, Manhattan, KS, United States
- 3School of Quantum Technology, DIAT(DU), Pune, India
An adaptive learning algorithm coupled with 3D momentum-based feedback is used to identify intense laser pulse shapes that control
1 Introduction
The intramolecular migration of hydrogen continues to be an active area of investigation in ultrafast science [1–11] with implications for topics ranging from combustion [12] to peptide dissociation [13] and characterizing conformational differences in molecules [14, 15]. In some cases the migration of hydrogen leads to the formation of new molecular ions, such as
The formation of
Ethane (C2H6) is composed of two back-to-back methyl groups, and thus it is an excellent baseline system for examining hydrogen-related bond rearrangement.
Motivated by significant
2 Experimental Method
The experimental techniques applied in this study have recently been discussed elsewhere [21, 36], and in this section we will only highlight a few key points. Two different approaches are used to examine the interactions of intense laser pulses with ethane gas: First, the laser pulses are shaped using an acousto-optic programmable dispersive filter (AOPDF) [37] and the ethane reaction products are measured using velocity map imaging (VMI) [38, 39]. Second, COLd Target Recoil Ion Momentum Spectroscopy (COLTRIMS) [40, 41] characterizes the dissociation dynamics of the ethane molecule following strong-field ionization.
2.1 Shaped Pulses and Velocity Map Imaging
In the shaped pulse/VMI portion of the experiment linearly polarized pulses with a duration of 35 fs full-width at half-maximum (FWHM) in intensity and a center wavelength of 785 nm are generated at 1 kHz by a Ti:Sapphire laser system named KLS. In this laser system, the compressor grating pair is in the Treacy configuration [42] while the stretcher gratings are in the Martinez configuration [43]. The amplified pulse energy of about 1.5 mJ was attenuated to the levels needed in the experiment. These near-Fourier-transform limited pulses will be denoted as TL pulses in this article. The acousto-optic programmable dispersive filter [37] was placed between the laser oscillator and multi-pass amplifier. In this experiment, we controlled only the spectral phase of the laser pulse. Pulse characteristics were determined using a second-harmonic-generation frequency-resolved-optical-grating (SHG-FROG) [44] device. Our version of VMI [45–47] integrates the momentum image of a given
FIGURE 1. Molecular fragmentation data obtained with 35 fs FWHM, 1.3
In the closed-loop adaptive control approach, ion-specific three-dimensional momentum information provides the feedback to drive a genetic algorithm that optimizes the pulse shapes to a control objective [46, 47]. The raw VMI data is inverted on-the-fly to recover a slice through the center of the three-dimensional momentum distribution using a modified “onion-peeling” algorithm as described by Rallis et al. [47]. The yield within user-defined regions of interest on the momentum plot is then evaluated, resulting in a numerical value that defines the “fitness” of the laser pulse being examined. The adaptive search parameterizes the pulse characteristics in terms of the spectral phase, which is broken into 16 evenly spaced segments between 734 and 830 nm. Since a portion of this range is beyond the pulse bandwidth, the effective number of search parameters is somewhat smaller than 16. Linear interpolation fills in the values between the adjacent phases. The algorithm is allowed to adjust each phase value between 0 and 2π.
To complement the closed-loop studies, systematic scans of the second- and third-order pulse dispersion were made for a few values of fourth-order dispersion. In this pulse-parameterization scheme [21, 50, 51], we describe the spectral phase,
2.2 Coincidence Momentum Imaging
In the COLTRIMS [40, 41] measurement, the laser pulses are produced by the PULSAR laser [53] at 10 kHz, with 25-fs (FWHM in intensity) pulse duration, a central wavelength of 790 nm, and maximum pulse energy of 2 mJ. The laser pulses were again characterized with SHG-FROG. The pulses are focused by a
3 Results and Discussion
The experiments on D3C-CH3 (1,1,1-d3 ethane, 98% pure) with shaped pulses and VMI detection used both an adaptive search strategy and a systematic search of pulse parameters. With this target,
As the intensity was increased, the VMI of the
FIGURE 2. (A) The red line shows the probability for two-body
3.1 Pulse Shaping and Control
We were able to increase the D2H+:
Figure 2 shows the KER distributions obtained for the D2H+ and
Notably, the D2H+ KER distribution obtained with the pulse optimized to increase the D2H+:
The characteristics of the optimized pulse are shown in Figure 3. While there is indeed a trailing secondary pulse around 125 fs after the main pulse, there are other features of the pulse shape that could be significant. To try and determine which pulse parameters are important for the manipulation of the control objective, we systematically scanned the linear chirp and third-order dispersion for three values of fourth-order dispersion. During these systematic scans we recorded the D2H+ and
FIGURE 3. (A) Measured frequency-resolved-optical-grating trace of the laser pulse optimized to increase the D2H+:
FIGURE 4. The yield of (A) D2H+ and (B)
From a time-domain perspective, the second–and fourth-order dispersions lengthen the pulse symmetrically, while the third-order dispersion adds a pedestal either before or after the main pulse (see, e.g., Ref. 50). Thus, some of the temporal characteristics of the optimized pulse (Figure 3) can be reproduced, but the secondary pulse would be more difficult to construct using dispersive pulse parameters. As shown in Figure 4C, there are a number of combinations of pulse parameters that reach nearly the same level of effectiveness at manipulating the D2H+:
One curious element of the dispersion scan is the comparison to the previous work of Schirmel et al., who also examined
One possible explanation for the seemingly conflicting results is that different intensities lead to different dissociation dynamics. The TL intensity of 1.3
3.2 Branching Ratio
Another factor potentially confounding our understanding of how the production of
FIGURE 5. The portion of the coincidence-time-of-flight map of two-body channels including
TABLE 1. Ethane (C2D6) branching ratios for two-body double ionization by 25-fs, 1.5
We also analyzed the three-body D +
Using momentum conservation to deduce the contribution from the deuterium atom gives a KER distribution for this three-body channel, shown in Figure 6. The KER distribution is similar to the
FIGURE 6. A comparison of the (COLTRIMS-derived) KER spectrum of
In addition, we did not find any significant evidence for
3.3 Angular Distributions
Since the control experiments with the D3C-CH3 isotopologue of ethane are designed to distinguish between the involvement of the hydrogen atoms on one or both sides of the molecule, the angular distributions from the VMI data might provide information about the dissociation dynamics beyond the KER shift shown in Figure 2B. Since the angular COLTRIMS data can be readily corrected using available experimental symmetries [36], we compared the COLTRIMS-measured
The angular distributions of the D2H+ and
FIGURE 7. The angular distributions of D2H+ and
TABLE 2. Legendre polynomial coefficients,
The optimized pulse, therefore, is observed to have a significant impact on the yield, KER, and angular distribution of the D2H+ ions. In contrast, the
4 Summary
By using the D3C-CH3 isotopologue of ethane we were able to separate two different types of dissociation processes leading to the formation of trihydrogen cations:
Data Availability Statement
The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.
Author Contributions
TT and TS led the analysis of the COLTRIMS measurements, while CS led the VMI analysis with assistance from TT, NI, and ST. BJ led the adaptive control experiments and KP led the dispersion scan experiments with assistance from NI, CS, JN, AS, TS, PF, ST, and EW. TS, BJ, SZ, KC, IB-I, and EW carried out the COLTRIMS experiment. IB-I and EW mentored the students and postdocs. EW wrote the manuscript with assistance from TT, TS, BJ, KP, KC, and IB-I. All authors reviewed the manuscript prior to submission.
Funding
Augustana University personnel and equipment are supported by the National Science Foundation grant PHYS-2011864. JR Macdonald Laboratory personnel and equipment are supported by the Chemical Sciences, Geosciences, and Biosciences Division, Office of Basic Energy Science, Office of Science, United States Department of Energy under award #DE-FG02-86ER1349.
Conflict of Interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Acknowledgments
We thank Charles Fehrenbach for assistance with the PULSAR laser and the members of Vinod Kumarappan’s group for assistance with the KLS laser.
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Keywords: coherent control, molecular dynamics, bond rearrangement, laser physics, imaging, ultrafast science
Citation: Townsend T, Schwartz CJ, Jochim B, P. KR, Severt T, Iwamoto N, Napierala JL, Feizollah P, Tegegn SN, Solomon A, Zhao S, Carnes KD, Ben-Itzhak I and Wells E (2021) Controlling
Received: 06 April 2021; Accepted: 10 June 2021;
Published: 30 June 2021.
Edited by:
Tamar Seideman, Northwestern University, United StatesReviewed by:
Arkaprabha Konar, Kent State University, United StatesBalakrishnan Naduvalath, University of Nevada, Las Vegas, United States
Copyright © 2021 Townsend, Schwartz, Jochim, P., Severt, Iwamoto, Napierala, Feizollah, Tegegn, Solomon, Zhao, Carnes, Ben-Itzhak and Wells. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: E. Wells, ZXJpYy53ZWxsc0BhdWdpZS5lZHU=