We present a protocol for probing ultrafast vibrational coherences in polyatomic radical cations that result in molecular dissociation.
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Method Article
We present a protocol for probing ultrafast vibrational coherences in polyatomic radical cations that result in molecular dissociation.
We present a pump-probe method for preparing vibrational coherences in polyatomic radical cations and probing their ultrafast dynamics. By shifting the wavelength of the strong-field ionizing pump pulse from the commonly used 800 nm into the near-infrared (1200-1600 nm), the contribution of adiabatic electron tunneling to the ionization process increases relative to multiphoton absorption. Adiabatic ionization results in predominant population of the ground electronic state of the ion upon electron removal, which effectively prepares a coherent vibrational state ("wave packet") amenable to subsequent excitation. In our experiments, the coherent vibrational dynamics are probed with a weak-field 800 nm pulse and the time-dependent yields of dissociation products measured in a time-of-flight mass spectrometer. We present the measurements on the molecule dimethyl methylphosphonate (DMMP) to illustrate how using 1500 nm pulses for excitation enhances the amplitude of coherent oscillations in ion yields by a factor of 10 as compared to 800 nm pulses. This protocol may be implemented in existing pump-probe setups through the incorporation of an optical parametric amplifier (OPA) for wavelength conversion.
Since the invention of the laser in 1960's, the goal of selectively breaking chemical bonds in molecules has been a longstanding dream of chemists and physicists. The ability to tune both laser frequency and intensity was believed to enable direct cleavage of a target bond through selective energy absorbance at the associated vibrational frequency1,2,3,4. However, early experiments found that intramolecular vibrational redistribution of the absorbed energy throughout the molecule often resulted in non-selective cleavage of the weakest bo....
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NOTE: All commercially acquired instruments and parts such as the laser, vacuum pumps, chamber, time-of-flight tube and microchannel plate detector were installed and operated according to the manufacturer’s instructions or user’s manual. Laser safety goggles designed for the operating laser intensities and wavelengths should be worn.
1. Construction of TOF-MS26
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Results obtained for the molecule DMMP21 are presented. Figure 3 shows the DMMP mass spectra taken at zero time-delay with the peak intensities of the 1500 nm pump and 800 nm probe pulses being 8 x 1013 and 8 x 1012 W cm-2, respectively. For reference, the mass spectrum taken with only the pump pulse is also shown. The spectra are averaged over 10,000 laser shots (total acquisition time 12 s). The incre.......
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This protocol enables us to resolve ultrafast vibrational dynamics in polyatomic radical cations through selective preparation of the ions in the ground electronic state. While the standard strong-field ionization procedure using 800 nm can prepare vibrational coherences in ground-electronic state radical cations of first-row diatomics10,11,12,13 and CO214
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The authors have nothing to disclose.
This work was supported by the U.S. Army Research Office through Contract W911NF-18-1-0051.
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| Name | Company | Catalog Number | Comments |
|---|---|---|---|
| Mass spectrometer components | |||
| TOF lens stack and flight tube assembly | Jordan TOF Products, Inc. | C-677 | |
| 18 mm Z-gap detector assembly | Jordan TOF Products, Inc. | C-701Z | |
| TOF high voltage power supply | Jordan TOF Products, Inc. | D-603 | |
| Vacuum system components | |||
| Rotary vane backing pump | Edwards Vacuum LLC | RV12 | |
| Turbomolecular pumps (2) | Edwards Vacuum LLC | EXT255H | |
| Turbomolecular pump controllers (2) | Edwards Vacuum LLC | EXC300 | |
| Pressure gauge | Edwards Vacuum LLC | AIGX-S-DN40CF | |
| Chiller for water cooling | Neslab | CFT-25 | |
| Femtosecond laser system | |||
| Ti:Sapphire regenerative amplifier | Coherent, Inc. | Astrella | oscillator and amplifier in a single integrated system |
| Optical Parametric Amplifer (OPA) | Light Conversion | TOPAS Prime | |
| Motion control | |||
| Motorized linear translation stage 1" travel | Thorlabs | Z825B | |
| controller for linear translation stage | Thorlabs | KDC 101 | |
| USB controller hub and power supply | Thorlabs | KCH 601 | |
| Manual linear translation stage 1" travel | Thorlabs | PT1 | |
| Detectors | |||
| Pyroelectric laser energy meter | Coherent, Inc. | 1168337 | |
| Thermal laser power meter | Coherent, Inc. | 5356E16R | |
| Si-biased detector 200-1100 nm | Thorlabs | DET10A | |
| Compact USB CMOS Camera | Thorlabs | DCC1545M | |
| USB spectrometer | Ocean Optics | HR4000 | |
| 1 GHz digital oscilloscope | LeCroy | WaveRunner 610Zi | |
| Optics | |||
| Type 1 BBO crystal | Crylight Photonics | BBO007 | aperture and thickness may be customized |
| Achromatic half wave plate, 1100-2000 nm | Thorlabs | AHWP05M-1600 | |
| Wollaston prism polarizer | Thorlabs | WPM10 | |
| Hollow retro-reflector | PLX, Inc. | OW-20-1C | |
| Variable neutral density filter | Thorlabs | NDC-100C-2 | |
| Longpass dichroic mirror 2" diameter | Thorlabs | DMLP950L | |
| Software | |||
| Digital Camera image software | Thorlabs | ThorCam | |
| Instrument communication interface | National Instruments | NI-MAX | |
| Graphical development environment for measurement programs | National Instruments | LabVIEW | |
| Data processing software | Mathworks | MATLAB |
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