Characterization of S <sub>2</sub> O and S <sub>2</sub> O <sup>–</sup> by Vibrational and Photoelectron Spectra Using a Quantum Mechanical Approach

In this work, accurate potential energy surfaces (PESs) of the neutral molecule S<sub>2</sub>O(X̃<sup>1</sup>A') and the anion S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) were constructed using high-level explicitly correlated CCSD(T)-F12 and MRCI-F12+Q methods with the cc-pCVQZ-F12 basis set, in which the PESs were represented by the neural network approach. Based on the PESs, we investigated the vibrational spectra of S<sub>2</sub>O(X̃<sup>1</sup>A') and S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″), the photoelectron spectrum of the S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) anion with hot bands, and associated isotope effects involving <sup>32</sup>S, <sup>33</sup>S, <sup>34</sup>S, <sup>36</sup>S, <sup>16</sup>O, and <sup>18</sup>O via a rigorous quantum mechanical approach. It was found that the calculated isotope ratios of S<sub>2</sub>O(X̃<sup>1</sup>A')/S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) and the photoelectron spectrum for <sup>32</sup>S<sub>2</sub><sup>16</sup>O<sup>-</sup> exhibit excellent agreement with experimental results. Associated isotope effects in the photoelectron spectrum are observed to be notably small, manifested by minor shifts in both peak positions and peak intensities. Vibrational wave function analysis reveals that the photoelectron spectrum of S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) is dominated by a strong vibrational progression, 3<sub>0</sub><sup><i>n</i></sup>, corresponding to the S-S stretching vibrational mode. Relatively weaker progressions are assigned to coupled vibrational states involving <i>v</i><sub>3</sub> (S-S stretching) and <i>v</i><sub>1</sub> (S-O stretching) modes, namely, the 3<sub>0</sub><sup><i>n</i></sup>1<sub>0</sub><sup>1</sup> and 3<sub>0</sub><sup><i>n</i></sup>1<sub>0</sub><sup>2</sup> progressions. The mode specificity in the photoelectron spectrum of S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) is qualitatively consistent with the relative amplitudes of the normal coordinate displacement (Δ<i>Q</i>) for vibrational modes during the ionization process.

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Journal
The Journal of Physical Chemistry A
Published
2025-12-03
DOI
https://doi.org/10.1021/acs.jpca.5c06663
Primary Topic
Advanced Chemical Physics Studies
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article
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article

Characterization of S 2 O and S 2 O – by Vibrational and Photoelectron Spectra Using a Quantum Mechanical Approach

Chunlei Teng, Bingbing Suo, Changjian Xie, Wenli Zou et al.
The Journal of Physical Chemistry A
Advanced Chemical Physics Studies
article

Characterization of S 2 O and S 2 O – by Vibrational and Photoelectron Spectra Using a Quantum Mechanical Approach

Chunlei Teng, Bingbing Suo, Changjian Xie, Wenli Zou, Huixian Han, Siting Hou
article en

Abstract

In this work, accurate potential energy surfaces (PESs) of the neutral molecule S<sub>2</sub>O(X̃<sup>1</sup>A') and the anion S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) were constructed using high-level explicitly correlated CCSD(T)-F12 and MRCI-F12+Q methods with the cc-pCVQZ-F12 basis set, in which the PESs were represented by the neural network approach. Based on the PESs, we investigated the vibrational spectra of S<sub>2</sub>O(X̃<sup>1</sup>A') and S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″), the photoelectron spectrum of the S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) anion with hot bands, and associated isotope effects involving <sup>32</sup>S, <sup>33</sup>S, <sup>34</sup>S, <sup>36</sup>S, <sup>16</sup>O, and <sup>18</sup>O via a rigorous quantum mechanical approach. It was found that the calculated isotope ratios of S<sub>2</sub>O(X̃<sup>1</sup>A')/S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) and the photoelectron spectrum for <sup>32</sup>S<sub>2</sub><sup>16</sup>O<sup>-</sup> exhibit excellent agreement with experimental results. Associated isotope effects in the photoelectron spectrum are observed to be notably small, manifested by minor shifts in both peak positions and peak intensities. Vibrational wave function analysis reveals that the photoelectron spectrum of S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) is dominated by a strong vibrational progression, 3<sub>0</sub><sup><i>n</i></sup>, corresponding to the S-S stretching vibrational mode. Relatively weaker progressions are assigned to coupled vibrational states involving <i>v</i><sub>3</sub> (S-S stretching) and <i>v</i><sub>1</sub> (S-O stretching) modes, namely, the 3<sub>0</sub><sup><i>n</i></sup>1<sub>0</sub><sup>1</sup> and 3<sub>0</sub><sup><i>n</i></sup>1<sub>0</sub><sup>2</sup> progressions. The mode specificity in the photoelectron spectrum of S<sub>2</sub>O<sup>-</sup>(X̃<sup>2</sup>A″) is qualitatively consistent with the relative amplitudes of the normal coordinate displacement (Δ<i>Q</i>) for vibrational modes during the ionization process.

The Journal of Physical Chemistry AVol. 129(50)
Northwest University (CN), Institute of Theoretical Physics (CN), Institute of Modern Physics (CN)
Openalex Percentile: Top 70%
Advanced Chemical Physics Studies
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