T J Herman, R Ravi, M S Schuurman, N J DeYonker, R W Field, L M Ziurys
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For the (4)<sup>2</sup>Σ<sup>+</sup> state, less intense spectra were recorded for <sup>24</sup>Mg<sup>35</sup>Cl (<i>v</i> = 0-2). Equilibrium rotational parameters were determined for both states for <sup>24</sup>Mg<sup>35</sup>Cl, as well as rotational constants and <sup>25</sup>Mg hyperfine parameters for the other isotopologues. A perturbation was observed between rotational levels of the two states due to an avoided crossing. Computations were also carried out at the CASPT2 and MRCISD+Q levels, and the resulting bond lengths for (3)<sup>2</sup>Σ<sup>+</sup> and (4)<sup>2</sup>Σ<sup>+</sup> states agree well with the experimental values of <i>r</i><sub>e</sub> = 2.536 and 2.361 Å. The computations show that the (3)<sup>2</sup>Σ<sup>+</sup> state has a double-well potential; however, the state behaves as a single well with unperturbed vibrational levels up to <i>v</i> = 13 due to nonadiabatic interactions with the (4)<sup>2</sup>Σ<sup>+</sup> state.</p>","PeriodicalId":59,"journal":{"name":"The Journal of Physical Chemistry A","volume":" ","pages":"9893-9903"},"PeriodicalIF":2.8000,"publicationDate":"2024-11-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11587948/pdf/","citationCount":"0","resultStr":"{\"title\":\"Probing the Electronic Manifold of MgCl with Millimeter-Wave Spectroscopy and Theory: (3)<sup>2</sup>Σ<sup>+</sup> and (4)<sup>2</sup>Σ<sup>+</sup> States.\",\"authors\":\"T J Herman, R Ravi, M S Schuurman, N J DeYonker, R W Field, L M Ziurys\",\"doi\":\"10.1021/acs.jpca.4c05458\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The millimeter/submillimeter spectrum of magnesium chloride (MgCl) has been observed in two new electronic excited states, (3)<sup>2</sup>Σ<sup>+</sup> and (4)<sup>2</sup>Σ<sup>+</sup>, using direct absorption methods. The molecule was synthesized in a mixture of Cl<sub>2</sub>, argon, and magnesium vapor. For the (3)<sup>2</sup>Σ<sup>+</sup> state, multiple rotational transitions were measured in the <i>v</i> = 0 level for all six isotopologues (<sup>24</sup>Mg<sup>35</sup>Cl, <sup>24</sup>Mg<sup>37</sup>Cl, <sup>25</sup>Mg<sup>35</sup>Cl, <sup>25</sup>Mg<sup>37</sup>Cl, <sup>26</sup>Mg<sup>35</sup>Cl, and <sup>26</sup>Mg<sup>37</sup>Cl), as well as up to <i>v</i> = 13 for <sup>24</sup>Mg<sup>35</sup>Cl. For the (4)<sup>2</sup>Σ<sup>+</sup> state, less intense spectra were recorded for <sup>24</sup>Mg<sup>35</sup>Cl (<i>v</i> = 0-2). Equilibrium rotational parameters were determined for both states for <sup>24</sup>Mg<sup>35</sup>Cl, as well as rotational constants and <sup>25</sup>Mg hyperfine parameters for the other isotopologues. A perturbation was observed between rotational levels of the two states due to an avoided crossing. Computations were also carried out at the CASPT2 and MRCISD+Q levels, and the resulting bond lengths for (3)<sup>2</sup>Σ<sup>+</sup> and (4)<sup>2</sup>Σ<sup>+</sup> states agree well with the experimental values of <i>r</i><sub>e</sub> = 2.536 and 2.361 Å. The computations show that the (3)<sup>2</sup>Σ<sup>+</sup> state has a double-well potential; however, the state behaves as a single well with unperturbed vibrational levels up to <i>v</i> = 13 due to nonadiabatic interactions with the (4)<sup>2</sup>Σ<sup>+</sup> state.</p>\",\"PeriodicalId\":59,\"journal\":{\"name\":\"The Journal of Physical Chemistry A\",\"volume\":\" \",\"pages\":\"9893-9903\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2024-11-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11587948/pdf/\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Journal of Physical Chemistry A\",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://doi.org/10.1021/acs.jpca.4c05458\",\"RegionNum\":2,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2024/11/13 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"Q3\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry A","FirstCategoryId":"1","ListUrlMain":"https://doi.org/10.1021/acs.jpca.4c05458","RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2024/11/13 0:00:00","PubModel":"Epub","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
摘要
利用直接吸收法观测到了氯化镁(MgCl)在两个新的电子激发态 (3)2Σ+ 和 (4)2Σ+ 中的毫米/亚毫米波谱。该分子是在 Cl2、氩气和镁蒸汽的混合物中合成的。对于 (3)2Σ+ 状态,在 v = 0 水平测量到了所有六种同位素(24Mg35Cl、24Mg37Cl、25Mg35Cl、25Mg37Cl、26Mg35Cl 和 26Mg37Cl)的多个旋转转变,以及 24Mg35Cl 的高达 v = 13 的旋转转变。对于 (4)2Σ+ 状态,24Mg35Cl(v = 0-2)的光谱强度较低。测定了 24Mg35Cl 两种状态的平衡旋转参数,以及其他同位素的旋转常数和 25Mg 超细参数。由于避免了交叉,在这两种状态的旋转水平之间观察到了扰动。计算还在 CASPT2 和 MRCISD+Q 水平上进行,得出的 (3)2Σ+ 和 (4)2Σ+ 状态的键长与实验值 re = 2.536 和 2.361 Å 非常吻合。计算结果表明,(3)2Σ+ 状态具有双阱势能;然而,由于与 (4)2Σ+ 状态的非绝热相互作用,该状态表现为单阱,其未受扰动的振动水平可达 v = 13。
Probing the Electronic Manifold of MgCl with Millimeter-Wave Spectroscopy and Theory: (3)2Σ+ and (4)2Σ+ States.
The millimeter/submillimeter spectrum of magnesium chloride (MgCl) has been observed in two new electronic excited states, (3)2Σ+ and (4)2Σ+, using direct absorption methods. The molecule was synthesized in a mixture of Cl2, argon, and magnesium vapor. For the (3)2Σ+ state, multiple rotational transitions were measured in the v = 0 level for all six isotopologues (24Mg35Cl, 24Mg37Cl, 25Mg35Cl, 25Mg37Cl, 26Mg35Cl, and 26Mg37Cl), as well as up to v = 13 for 24Mg35Cl. For the (4)2Σ+ state, less intense spectra were recorded for 24Mg35Cl (v = 0-2). Equilibrium rotational parameters were determined for both states for 24Mg35Cl, as well as rotational constants and 25Mg hyperfine parameters for the other isotopologues. A perturbation was observed between rotational levels of the two states due to an avoided crossing. Computations were also carried out at the CASPT2 and MRCISD+Q levels, and the resulting bond lengths for (3)2Σ+ and (4)2Σ+ states agree well with the experimental values of re = 2.536 and 2.361 Å. The computations show that the (3)2Σ+ state has a double-well potential; however, the state behaves as a single well with unperturbed vibrational levels up to v = 13 due to nonadiabatic interactions with the (4)2Σ+ state.
期刊介绍:
The Journal of Physical Chemistry A is devoted to reporting new and original experimental and theoretical basic research of interest to physical chemists, biophysical chemists, and chemical physicists.