{"title":"O2(Σg−3)-SO2 (1A1)开壳二聚体的新光谱拟合和从头计算研究","authors":"Wafaa M. Fawzy","doi":"10.1016/j.jms.2025.112010","DOIUrl":null,"url":null,"abstract":"<div><div>We report the first accurate global fits for the rotation-spin-tunneling transitions in the microwave spectrum of the O<sub>2</sub>(<span><math><mmultiscripts><msubsup><mi>Σ</mi><mi>g</mi><mo>−</mo></msubsup><mprescripts></mprescripts><mspace></mspace><mn>3</mn></mmultiscripts></math></span>)-SO<sub>2</sub> (<sup>1</sup>A<sub>1</sub>) weakly bonded open-shell complex. In addition, we present a new ab initio investigation of the potential energy surface of O<sub>2</sub>(<span><math><mmultiscripts><msubsup><mi>Σ</mi><mi>g</mi><mo>−</mo></msubsup><mprescripts></mprescripts><mspace></mspace><mn>3</mn></mmultiscripts></math></span>)-SO<sub>2</sub>, using the UCCSD(T)/aug-cc-pV(n + d)Z level of theory where <em>n</em> = 2 and 3. Analysis of the spectrum identified a-type and c-type transitions, frequencies of the a-type were not shifted while those of the c-type were shifted due to tunneling of the O<sub>2</sub> and the SO<sub>2</sub> moieties in the dimer. Only the A<sub>1</sub> symmetric tunneling state was detected because the antisymmetric A<sub>2</sub> state is not allowed by nuclear spin statistics in O<sub>2</sub>-SO<sub>2</sub>. Least squares fits with a standard deviation of 1 kHz were obtained using two computer codes incorporating semi-rigid rotor Hamiltonians that employ two different angular momenta coupling schemes. Results of the fits determined the effective tunneling frequency in the A<sub>1</sub> symmetric state as <span><math><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>= 2373.61134 <span><math><mo>±</mo></math></span>16 MHz, the electron spin coupling constant λ = 42,870.2186 <span><math><mo>±</mo></math></span>43 MHz, the rotational constants A = 7099.44 <span><math><mo>±</mo></math></span>33, B = 1528.886 <span><math><mo>±</mo></math></span>5, C = 1763.36 <span><math><mo>±</mo></math></span>6 MHz. The value of <span><math><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span> equals the tunneling splitting (<span><math><msub><mi>Δ</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>) between the<span><math><msubsup><mi>A</mi><mn>1</mn><mo>+</mo></msubsup></math></span> and <span><math><msubsup><mi>A</mi><mn>1</mn><mo>−</mo></msubsup></math></span> symmetric tunneling states in the dimer, where the<span><math><msubsup><mi>A</mi><mn>1</mn><mo>+</mo></msubsup></math></span> and <span><math><msubsup><mi>A</mi><mn>1</mn><mo>−</mo></msubsup></math></span> levels are shifted in energy by <span><math><mo>−</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span> and <span><math><mo>+</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>, respectively. The ab initio study identified a global minimum energy structure of C<sub>1</sub> symmetry and a metastable local minimum of C<sub>s</sub> symmetry. We computed the optimized geometries of four equivalent configurations in the minimum energy isomer, which are due to rotation-tunneling motion of each monomer and concerted tunneling of the subunits in the dimer. A structure of C<sub>2v</sub> symmetry was determined as the transition state between the concerted tunneling minima with a barrier height of 77.8 cm<sup>−1</sup>. The binding energy in the global minimum was calculated with the BSSE correction as 2.676 kcal/mol. Results of the spectroscopic fits are in excellent agreement with those obtained from our ab initio calculations.</div></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"409 ","pages":"Article 112010"},"PeriodicalIF":1.4000,"publicationDate":"2025-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"New spectroscopic fits and ab initio study of the O2(Σg−3)-SO2 (1A1) open-shell dimer\",\"authors\":\"Wafaa M. Fawzy\",\"doi\":\"10.1016/j.jms.2025.112010\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We report the first accurate global fits for the rotation-spin-tunneling transitions in the microwave spectrum of the O<sub>2</sub>(<span><math><mmultiscripts><msubsup><mi>Σ</mi><mi>g</mi><mo>−</mo></msubsup><mprescripts></mprescripts><mspace></mspace><mn>3</mn></mmultiscripts></math></span>)-SO<sub>2</sub> (<sup>1</sup>A<sub>1</sub>) weakly bonded open-shell complex. In addition, we present a new ab initio investigation of the potential energy surface of O<sub>2</sub>(<span><math><mmultiscripts><msubsup><mi>Σ</mi><mi>g</mi><mo>−</mo></msubsup><mprescripts></mprescripts><mspace></mspace><mn>3</mn></mmultiscripts></math></span>)-SO<sub>2</sub>, using the UCCSD(T)/aug-cc-pV(n + d)Z level of theory where <em>n</em> = 2 and 3. Analysis of the spectrum identified a-type and c-type transitions, frequencies of the a-type were not shifted while those of the c-type were shifted due to tunneling of the O<sub>2</sub> and the SO<sub>2</sub> moieties in the dimer. Only the A<sub>1</sub> symmetric tunneling state was detected because the antisymmetric A<sub>2</sub> state is not allowed by nuclear spin statistics in O<sub>2</sub>-SO<sub>2</sub>. Least squares fits with a standard deviation of 1 kHz were obtained using two computer codes incorporating semi-rigid rotor Hamiltonians that employ two different angular momenta coupling schemes. Results of the fits determined the effective tunneling frequency in the A<sub>1</sub> symmetric state as <span><math><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>= 2373.61134 <span><math><mo>±</mo></math></span>16 MHz, the electron spin coupling constant λ = 42,870.2186 <span><math><mo>±</mo></math></span>43 MHz, the rotational constants A = 7099.44 <span><math><mo>±</mo></math></span>33, B = 1528.886 <span><math><mo>±</mo></math></span>5, C = 1763.36 <span><math><mo>±</mo></math></span>6 MHz. The value of <span><math><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span> equals the tunneling splitting (<span><math><msub><mi>Δ</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>) between the<span><math><msubsup><mi>A</mi><mn>1</mn><mo>+</mo></msubsup></math></span> and <span><math><msubsup><mi>A</mi><mn>1</mn><mo>−</mo></msubsup></math></span> symmetric tunneling states in the dimer, where the<span><math><msubsup><mi>A</mi><mn>1</mn><mo>+</mo></msubsup></math></span> and <span><math><msubsup><mi>A</mi><mn>1</mn><mo>−</mo></msubsup></math></span> levels are shifted in energy by <span><math><mo>−</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span> and <span><math><mo>+</mo><mfrac><mn>1</mn><mn>2</mn></mfrac><msub><mi>ν</mi><msub><mi>T</mi><mn>1</mn></msub></msub></math></span>, respectively. The ab initio study identified a global minimum energy structure of C<sub>1</sub> symmetry and a metastable local minimum of C<sub>s</sub> symmetry. We computed the optimized geometries of four equivalent configurations in the minimum energy isomer, which are due to rotation-tunneling motion of each monomer and concerted tunneling of the subunits in the dimer. A structure of C<sub>2v</sub> symmetry was determined as the transition state between the concerted tunneling minima with a barrier height of 77.8 cm<sup>−1</sup>. The binding energy in the global minimum was calculated with the BSSE correction as 2.676 kcal/mol. Results of the spectroscopic fits are in excellent agreement with those obtained from our ab initio calculations.</div></div>\",\"PeriodicalId\":16367,\"journal\":{\"name\":\"Journal of Molecular Spectroscopy\",\"volume\":\"409 \",\"pages\":\"Article 112010\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2025-03-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Molecular Spectroscopy\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0022285225000268\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"PHYSICS, ATOMIC, MOLECULAR & CHEMICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Molecular Spectroscopy","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022285225000268","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"PHYSICS, ATOMIC, MOLECULAR & CHEMICAL","Score":null,"Total":0}
New spectroscopic fits and ab initio study of the O2(Σg−3)-SO2 (1A1) open-shell dimer
We report the first accurate global fits for the rotation-spin-tunneling transitions in the microwave spectrum of the O2()-SO2 (1A1) weakly bonded open-shell complex. In addition, we present a new ab initio investigation of the potential energy surface of O2()-SO2, using the UCCSD(T)/aug-cc-pV(n + d)Z level of theory where n = 2 and 3. Analysis of the spectrum identified a-type and c-type transitions, frequencies of the a-type were not shifted while those of the c-type were shifted due to tunneling of the O2 and the SO2 moieties in the dimer. Only the A1 symmetric tunneling state was detected because the antisymmetric A2 state is not allowed by nuclear spin statistics in O2-SO2. Least squares fits with a standard deviation of 1 kHz were obtained using two computer codes incorporating semi-rigid rotor Hamiltonians that employ two different angular momenta coupling schemes. Results of the fits determined the effective tunneling frequency in the A1 symmetric state as = 2373.61134 16 MHz, the electron spin coupling constant λ = 42,870.2186 43 MHz, the rotational constants A = 7099.44 33, B = 1528.886 5, C = 1763.36 6 MHz. The value of equals the tunneling splitting () between the and symmetric tunneling states in the dimer, where the and levels are shifted in energy by and , respectively. The ab initio study identified a global minimum energy structure of C1 symmetry and a metastable local minimum of Cs symmetry. We computed the optimized geometries of four equivalent configurations in the minimum energy isomer, which are due to rotation-tunneling motion of each monomer and concerted tunneling of the subunits in the dimer. A structure of C2v symmetry was determined as the transition state between the concerted tunneling minima with a barrier height of 77.8 cm−1. The binding energy in the global minimum was calculated with the BSSE correction as 2.676 kcal/mol. Results of the spectroscopic fits are in excellent agreement with those obtained from our ab initio calculations.
期刊介绍:
The Journal of Molecular Spectroscopy presents experimental and theoretical articles on all subjects relevant to molecular spectroscopy and its modern applications. An international medium for the publication of some of the most significant research in the field, the Journal of Molecular Spectroscopy is an invaluable resource for astrophysicists, chemists, physicists, engineers, and others involved in molecular spectroscopy research and practice.