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    <identifier>10.57760/sciencedb.j00213.00058</identifier>
    <datestamp>2024-10-18T17:30:34Z</datestamp>
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<oai_dc:dc 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" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2024-10-18</dc:date>
  <dc:title>Theoretical investigation on spectroscopic characteristics of 14 &amp;Lambda;-S and 27 &amp;Omega; states of OH+ cations</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.j00213.00058</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>Based on theoretical frameworks such as icMRCI+Q and the accurate treatment of scalar relativistic effect, core-valence electron correlation, complete basis set limit, and spin-orbit coupling effect, this article calculates the relevant spectroscopic and vibrational-rotational transition data for 14 &amp;Lambda;-S and 27 &amp;Omega; states of OH+ cation. The dataset includes potential energy curves of 14 &amp;Lambda;-S and 27 &amp;Omega; states, 7 pairs of transition dipole moments between the 6 &amp;Omega; states [X3&amp;Sigma;-0+, X3&amp;Sigma;-1, (1)2, (2)2, (2)1, (1)0-], and distributions of the radiative lifetime varying as the J' of the (2)21st well(&amp;upsilon;' = 0 &amp;minus; 2, +), (2)1(&amp;upsilon;' = 0&amp;minus;9, +), and (1)0-(&amp;upsilon;' = 0&amp;minus;8, +) states. Based on the potential energy curves and transition dipole moments mentioned above, by solving the vibrational-rotational Schr&amp;ouml;dinger equation for nuclear motion and the formulas (1-4) in the article, we obtained the spectroscopic constants (Te, Re, &amp;omega;e, &amp;omega;exe, Be, &amp;alpha;e, D0, and De) and molecular constants for 12 &amp;Lambda;-S and 27 &amp;Omega; bound and weakly bound states, the vibrational-rotational transition data for the seven pairs of transitions between X3&amp;Sigma;-0+, X3&amp;Sigma;-1, (1)2(&amp;upsilon;' = 0&amp;ndash;6), (2)21st well(&amp;upsilon;' = 0&amp;ndash;2), (2)1(&amp;upsilon;'&amp;nbsp;= 0&amp;ndash;9), and (1)0-(&amp;upsilon;' = 0&amp;ndash;8) states with less perturbation by other &amp;Omega; states, such as the transition wave numbers, Einstein A coefficients, vibrational branching ratios, weighted absorption oscillator strengths, wavelengths, radiation lifetimes and radiation widths of four excited &amp;Omega; states[(1)2(&amp;upsilon;' = 0&amp;minus;6, J' = 2, +), (2)21st well(&amp;upsilon;' = 0&amp;minus;2, J' = 2, +), (2)1(&amp;upsilon;' = 0&amp;minus;9, J' = 1, +), and (1)0-(&amp;upsilon;' = 0&amp;minus;8, J' = 0, +)].</dc:description>
  <dc:subject>icMRCI+Q method; spin-orbit coupling; potential energy curves; transition dipole moments</dc:subject>
  <dc:creator>xing wei</dc:creator>
  <dc:creator>Li Shengzhou</dc:creator>
  <dc:creator>Zhang Fang</dc:creator>
  <dc:creator>Sun Jinfeng</dc:creator>
  <dc:creator>Li Wentao</dc:creator>
  <dc:creator>Zhu Zunlüe</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/10.7498/aps.73.20241301</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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