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    <responseDate>2026-10-10T07:20:17Z</responseDate>
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                <identifier>oai:data.mendeley.com/b99tndkk99.1</identifier>
                <datestamp>2023-11-06T15:11:18Z</datestamp>
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            <metadata><oai_dc:dc xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
    <dc:creator>Sarka, Karolis</dc:creator>
    <dc:title>Potential energy curves and UV absorption cross-sections of sulfur dimer</dc:title>
    <dc:publisher>Mendeley Data</dc:publisher>
    <dc:description>MRCI-F12+Q/aug-cc-pV(5+d)Z ab initio potential energy and transition dipole moment curves of three S2 electronic states: X^3\Sigma_g^-, B&apos;&apos;^3\Pi_u (both x,y degeneracies), B^3\Sigma_u^-.

In addition, absorption cross-sections are included for four isotopologues (32S32S, 33S32S, 34S32S, and 36S32S) at T=300K. Additional two absorption cross-sections are included for 32S32S at T=370K and 823K for comparison with experimental cross-sections produced by Stark et al., J. Chem. Phys. 148, 244302 (2018).

The absorption cross-sections are in cm^2 and the wavelength is in nm. Potential energy curves are in Hartree and interatomic distance is in Aangstrom.

For linelists, the filename convention is used as follows:
discrete_[excited electronic state e]_[ground electronic v]_[ground electronic J].dat
for all discrete transitions from the specific v,J state to e. Indices are 0: B&apos;&apos;^3Pi_ux; 1: B&apos;&apos;^3Pi_uy; 2: B^3sigma_u^-

The linelist contents are displayed in two main columns:
[Energy (Hartree), Cross-section (cm^2)]
and for the B^3sigma_u^- state, i.e. discrete_2_i_j.dat files:
[Energy (Hartree), Cross-section (cm^2), Gamma (cm^-1)]
where Gamma is the pre-dissociation FWHM broadening factor for states with energy greater than the dissociation energy for B&apos;&apos;^3Pi_u state.

The factor Gamma is calculated according to the close-coupling method shown in van Dischoeck et al. (1984), https://doi.org/10.1063/1.447622.

However, we are not certain with the complete accuracy of it, since we have not included spin-orbit coupling interactions, which is expected to have an effect on the pre-dissociation factor.

continuum_[excited electronic state e]_[ground electronic v]_[ground electronic J].dat
for evenly spaced continuum transitions from the specific v,J state to e. Indices are 0: B Pi_ux; 1: B Pi_uy; 2: B_sigma_u
[Energy (Hartree), Cross-section (cm^2)]

gnd_energies.dat
for all ground state v, J levels
[v, J, Energy (Hartree)]


The attached python script total_csection.py can be used to reproduce the total absorption cross-sections from linelists for each isotopologue by renaming the linelist directory to &apos;results&apos; and putting in the same working directory as the script. Invoking the script, e.g.:
&gt;&gt;python3 total_csection.py --recalc --temp 300 --isos 32S 32S 
will produce the total absorption cross-section with Boltzmann distribution and Doppler broadening at 300 Kelvin for 32S32S molecule.</dc:description>
    <dc:subject>Theoretical Chemistry</dc:subject>
    <dc:subject>Absorption Spectroscopy</dc:subject>
    <dc:subject>Potential Energy Surface</dc:subject>
    <dc:contributor>Nanbu, Shinkoh</dc:contributor>
    <dc:type>Dataset</dc:type>
    <dc:identifier>doi:10.17632/b99tndkk99.1</dc:identifier>
    <dc:identifier>oai:data.mendeley.com/b99tndkk99.1</dc:identifier>
    <dc:rights>Creative Commons Attribution 4.0 International</dc:rights>
    <dc:rights>http://creativecommons.org/licenses/by/4.0</dc:rights>
    <dc:relation>https://data.mendeley.com/datasets/b99tndkk99</dc:relation>
    <dc:date>2023-11-06T15:11:18Z</dc:date>
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