Pub Date : 2024-02-01DOI: 10.1016/j.jms.2023.111871
Yoshiyuki Kawashima , Nobuhiko Kuze , Koichi M. T. Yamada , Eizi Hirota
We observed ten pseudo a-type transitions in the E state of N-ethylacetamide (NEAA) using a Fourier transform microwave spectrometer. We found triplets caused by the coupling between the two methyl groups for the observed pseudo a-type transitions. Also, we succeeded in observing similar triplets for the 5 a-type Q-branch transitions, 20 b-type and 7 c-type transitions of the E state of NEAA. These observed triplets allowed us to determinate the potential barrier V3 to internal rotation of the ethyl-methyl group to be 1078 (12) cm−1. In addition, though the observed intensities of the c-type transitions in the A state were weak, the c-type transition in the E state were observed to be as intense as the b-type transitions of the E state. We explained in this paper the abnormal intensities of the c-type transitions and pseudo a-type transitions in the E state of NEAA.
我们使用傅立叶变换微波光谱仪观测到了 N-乙基乙酰胺(NEAA)E 态的十个伪 a 型跃迁。我们发现,在观测到的伪 a 型跃迁中,两个甲基之间的耦合引起了三连串。此外,我们还成功地观测到了 NEAA E 态的 5 个 a 型 Q 支转变、20 个 b 型转变和 7 个 c 型转变的类似三连串。通过这些观察到的三连串,我们确定了乙基甲基内旋转的势垒 V3 为 1078 (12) cm-1。此外,虽然在 A 态中观察到的 c 型转变强度很弱,但在 E 态中观察到的 c 型转变强度与 E 态的 b 型转变强度相当。我们在本文中解释了东北亚大气中 E 态 c 型转变和伪 a 型转变的异常强度。
{"title":"Reinvestigation of the Fourier transform microwave spectrum of N-ethylacetamide: Pseudo a-type transitions","authors":"Yoshiyuki Kawashima , Nobuhiko Kuze , Koichi M. T. Yamada , Eizi Hirota","doi":"10.1016/j.jms.2023.111871","DOIUrl":"10.1016/j.jms.2023.111871","url":null,"abstract":"<div><p>We observed ten pseudo <em>a</em>-type transitions in the <em>E</em> state of <em>N</em>-ethylacetamide (NEAA) using a Fourier transform microwave spectrometer. We found triplets caused by the coupling between the two methyl groups for the observed pseudo <em>a</em>-type transitions. Also, we succeeded in observing similar triplets for the 5 <em>a</em>-type <em>Q</em>-branch transitions, 20 <em>b</em>-type and 7 <em>c</em>-type transitions of the <em>E</em> state of NEAA. These observed triplets allowed us to determinate the potential barrier <em>V</em><sub>3</sub> to internal rotation of the ethyl-methyl group to be 1078 (12) cm<sup>−1</sup>. In addition, though the observed intensities of the <em>c</em>-type transitions in the <em>A</em> state were weak, the <em>c</em>-type transition in the <em>E</em> state were observed to be as intense as the <em>b</em>-type transitions of the <em>E</em> state. We explained in this paper the abnormal intensities of the <em>c</em>-type transitions and pseudo <em>a</em>-type transitions in the <em>E</em> state of NEAA.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111871"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138692987","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.jms.2024.111889
Jan Suchánek , Michal Dostál , Václav Nevrlý , Pavel Kubát , Hana Chaloupecká , Zdeněk Zelinger
Cantilever-enhanced Photoacoustic Spectroscopy in combination with Wavelength Modulation Spectroscopy was used for the multicomponent analysis of gases. Distributed feedback Quantum Cascade Laser tunable in the region of ∼ 1045 – 1048 cm−1 was used as the excitation source. Principal component analysis (PCA) and Partial Least Squares (PLS) (the pls package in the statistical software R) methods were applied to a mixture of selected substances (methanol and ethanol) in the gas phase to both simulated (www.spectraplot.com) and experimentally acquired spectra, PCA predicting the number of substances and PLS its concentrations.
{"title":"Chemometrics approach to Cantilever enhanced photoacoustic spectroscopy with Quantum Cascade lasers","authors":"Jan Suchánek , Michal Dostál , Václav Nevrlý , Pavel Kubát , Hana Chaloupecká , Zdeněk Zelinger","doi":"10.1016/j.jms.2024.111889","DOIUrl":"https://doi.org/10.1016/j.jms.2024.111889","url":null,"abstract":"<div><p>Cantilever-enhanced Photoacoustic Spectroscopy in combination with Wavelength Modulation Spectroscopy was used for the multicomponent analysis of gases. Distributed feedback Quantum Cascade Laser tunable in the region of ∼ 1045 – 1048 cm<sup>−1</sup> was used as the excitation source. Principal component analysis (PCA) and Partial Least Squares (PLS) (the pls package in the statistical software R) methods were applied to a mixture of selected substances (methanol and ethanol) in the gas phase to both simulated (<span>www.spectraplot.com</span><svg><path></path></svg>) and experimentally acquired spectra, PCA predicting the number of substances and PLS its concentrations.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111889"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139898733","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.jms.2024.111890
Youquan Yang , Zhimin Peng , Dao Zheng , Meng Zhang , Yanjun Ding , Yanjun Du
Line strengths and line shape parameters of Ar- and N2-perturbed CO2 R-branch transitions (82 90) in the fundamental band were measured in a shock tube from 730 K to 2500 K and pressure below 1.13 atm using laser absorption spectroscopy (LAS). The retrieved absorption curves were fitted with the Voigt and the quadratic speed-dependent Voigt (qSDV) profiles to obtain the line strengths, broadening, and shift coefficients. Line strengths were compared to values in HITEMP, HITRAN2020, and Ames2021 databases, and the HITEMP shows the best agreement with the measured results. Ar- and N2-broadening and shift coefficients were regressed into the power law and the double power law form to study the temperature dependence of the targeted lines. The speed-dependence parameter was temperature-dependent. The J-dependence of the derived broadening and shift coefficients was discussed. The results of this work will aid the development of the absorption model in the far-wing region and the design of CO2 LAS sensors for high-temperature measurement.
利用激光吸收光谱(LAS)测量了在 730 K 至 2500 K、压力低于 1.13 atm 的冲击管中,ν3 基带中 Ar 和 N2 扰动的 CO2 R 分支跃迁(82 ≤J″≤ 90)的线强度和线形参数。用 Voigt 和二次速度依赖性 Voigt(qSDV)曲线拟合得到的吸收曲线,从而获得了线强度、展宽和位移系数。线强度与 HITEMP、HITRAN2020 和 Ames2021 数据库中的值进行了比较,结果表明 HITEMP 与测量结果的一致性最好。将氩气和氮气的增宽和位移系数回归为幂律和双幂律形式,以研究目标线的温度依赖性。速度相关参数 aw 与温度有关。讨论了得出的增宽和位移系数的 J 依赖性。这项工作的结果将有助于开发远翼区吸收模型和设计用于高温测量的 CO2 LAS 传感器。
{"title":"High-temperature line strength and line shape parameters measurements of Ar- and N2-perturbed CO2 lines near 4.18 µm in a shock tube","authors":"Youquan Yang , Zhimin Peng , Dao Zheng , Meng Zhang , Yanjun Ding , Yanjun Du","doi":"10.1016/j.jms.2024.111890","DOIUrl":"10.1016/j.jms.2024.111890","url":null,"abstract":"<div><p>Line strengths and line shape parameters of Ar- and N<sub>2</sub>-perturbed CO<sub>2</sub> R-branch transitions (82 <span><math><mrow><mo>≤</mo><msup><mrow><mi>J</mi></mrow><mo>″</mo></msup><mo>≤</mo></mrow></math></span> 90) in the <span><math><mrow><msub><mi>ν</mi><mn>3</mn></msub></mrow></math></span> fundamental band were measured in a shock tube from 730 K to 2500 K and pressure below 1.13 atm using laser absorption spectroscopy (LAS). The retrieved absorption curves were fitted with the Voigt and the quadratic speed-dependent Voigt (qSDV) profiles to obtain the line strengths, broadening, and shift coefficients. Line strengths were compared to values in HITEMP, HITRAN2020, and Ames2021 databases, and the HITEMP shows the best agreement with the measured results. Ar- and N<sub>2</sub>-broadening and shift coefficients were regressed into the power law and the double power law form to study the temperature dependence of the targeted lines. The speed-dependence parameter <span><math><mrow><msub><mi>a</mi><mi>w</mi></msub></mrow></math></span> was temperature-dependent. The <em>J</em>-dependence of the derived broadening and shift coefficients was discussed. The results of this work will aid the development of the absorption model in the far-wing region and the design of CO<sub>2</sub> LAS sensors for high-temperature measurement.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111890"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139954205","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-17DOI: 10.1016/j.jms.2024.111884
Kristen K. Roehling, Rhett P. Hill, Adam M. Daly, Stephen G. Kukolich
New analysis and spectra are reported for the gas-phase ammonia-formic acid complex. Calculations to determine the theoretical barrier to internal rotation were conducted and led to the new internal rotation analysis of the dimer. Using the new analysis and calculations, 12 new lines were measured and assigned and included in the present analysis. This is the first internal rotation analysis for this complex. The measurements were made in the 7–22 GHz range using two Flygare-Balle type pulsed beam Fourier transform microwave (FTMW) spectrometers. The complex was analyzed as a hindered rotor and 20 A and 16 E state transitions were fit with the XIAM5 program. The rotational constants were determined to have the following values: A = 11970.19(9) MHz, B = 4331.479(4) MHz, and C = 3227.144(4) MHz. Rotational constants, quadrupole coupling constants, and internal rotor parameters were fit to the spectrum. Double resonance was used to verify line assignments and access higher frequencies. The barrier to internal rotation was found to be 195.18(7) cm−1. High level calculations are in good agreement with experimental values. The calculated V3 barrier values range from 168.3 to 212.8 cm−1.
{"title":"Ammonia – Formic acid complex: internal rotation analysis, calculations, and new microwave measurements","authors":"Kristen K. Roehling, Rhett P. Hill, Adam M. Daly, Stephen G. Kukolich","doi":"10.1016/j.jms.2024.111884","DOIUrl":"10.1016/j.jms.2024.111884","url":null,"abstract":"<div><p>New analysis and spectra are reported for the gas-phase ammonia-formic acid complex. Calculations to determine the theoretical barrier to internal rotation were conducted and led to the new internal rotation analysis of the dimer. Using the new analysis and calculations, 12 new lines were measured and assigned and included in the present analysis. This is the first internal rotation analysis for this complex. The measurements were made in the 7–22 GHz range using two Flygare-Balle type pulsed beam Fourier transform microwave (FTMW) spectrometers. The complex was analyzed as a hindered rotor and 20 A and 16 E state transitions were fit with the XIAM5 program. The rotational constants were determined to have the following values: A = 11970.19(9) MHz, B = 4331.479(4) MHz, and C = 3227.144(4) MHz. Rotational constants, quadrupole coupling constants, and internal rotor parameters were fit to the spectrum. Double resonance was used to verify line assignments and access higher frequencies. The barrier to internal rotation was found to be 195.18(7) cm<sup>−1</sup>. High level calculations are in good agreement with experimental values. The calculated V<sub>3</sub> barrier values range from 168.3 to 212.8 cm<sup>−1</sup>.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111884"},"PeriodicalIF":1.4,"publicationDate":"2024-01-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139496437","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-17DOI: 10.1016/j.jms.2024.111885
A. Jusuf, T.L. Tan
A total of 11 fundamental and 3 overtone bands of the formaldoxime isotopologue 13CD2NOH were identified using its Fourier transform infrared (FTIR) spectra which were recorded with a low resolution (0.50 cm−1) in the 500–4000 cm−1 region, and high resolution (0.00096 cm−1) in the 280–500 cm−1 region. Their relative infrared (IR) band intensities were also measured. Furthermore, a rovibrational analysis of the IR transitions of the band of 13CD2NOH was carried out using its high-resolution FTIR spectrum which was recorded at the Australian Synchrotron. A total of 1077 IR transitions of the C-type band were assigned and fitted using the Watson's A-reduced Hamiltonian in the Ir representation to derive its band center and the = 1 state rovibrational constants up to all 5 quartic centrifugal distortion terms for the first time, with a root-mean-square (rms) deviation of 0.00044 cm−1. The band center of the band of 13CD2NOH were found to be 391.054446(36) cm−1. The ground state rovibrational constants up to all 5 quartic terms were determined for the first time by fitting 407 ground state combination differences (GSCDs) derived from the assigned IR transitions of the band of 13CD2NOH of this work. The rms deviation of the GSCD fit was 0.00040 cm−1. Additionally, all 3 rotational constants and 5 quartic centrifugal distortion terms of the ground state and 3 rotational constants of the = 1 state of 13CD2NOH were computed from theoretical anharmonic calculations at two different levels of theory, B3LYP and MP2 with the cc-pVTZ basis set, for comparison with the experimental results. Close agreement was found for the calculated and experimental rovibrational constants of 13CD2NOH for both ground and = 1 states. The vibrational anharmonic frequencies of the 12 fundamental bands of 13CD2NOH in the 280–4000 cm−1 region, and their IR band intensities were also calculated using B3LYP and MP2 with the cc-pVTZ basis set, and they were compared with the respective experimental data. Finally, the ground state rotational constants and the band center of the
{"title":"Vibrational bands of formaldoxime isotopologue 13CD2NOH in the 280–4000 cm−1 region and rovibrational analysis of its ν12 band by Fourier transform infrared (FTIR) spectroscopy","authors":"A. Jusuf, T.L. Tan","doi":"10.1016/j.jms.2024.111885","DOIUrl":"10.1016/j.jms.2024.111885","url":null,"abstract":"<div><p>A total of 11 fundamental and 3 overtone bands of the formaldoxime isotopologue <sup>13</sup>CD<sub>2</sub>NOH were identified using its Fourier transform infrared (FTIR) spectra which were recorded with a low resolution (0.50 cm<sup>−1</sup>) in the 500–4000 cm<sup>−1</sup> region, and high resolution (0.00096 cm<sup>−1</sup>) in the 280–500 cm<sup>−1</sup> region. Their relative infrared (IR) band intensities were also measured. Furthermore, a rovibrational analysis of the IR transitions of the <span><math><mrow><msub><mi>ν</mi><mn>12</mn></msub></mrow></math></span> band of <sup>13</sup>CD<sub>2</sub><span>NOH was carried out using its high-resolution FTIR spectrum which was recorded at the Australian Synchrotron. A total of 1077 IR transitions of the </span><em>C</em>-type <span><math><mrow><msub><mi>ν</mi><mn>12</mn></msub></mrow></math></span> band were assigned and fitted using the Watson's <em>A</em>-reduced Hamiltonian in the <em>I<sup>r</sup></em> representation to derive its band center and the <span><math><mrow><msub><mi>v</mi><mn>12</mn></msub></mrow></math></span><span> = 1 state rovibrational constants up to all 5 quartic centrifugal distortion terms for the first time, with a root-mean-square (rms) deviation of 0.00044 cm</span><sup>−1</sup>. The band center of the <span><math><mrow><msub><mi>ν</mi><mn>12</mn></msub></mrow></math></span> band of <sup>13</sup>CD<sub>2</sub>NOH were found to be 391.054446(36) cm<sup>−1</sup>. The ground state rovibrational constants up to all 5 quartic terms were determined for the first time by fitting 407 ground state combination differences (GSCDs) derived from the assigned IR transitions of the <span><math><mrow><msub><mi>ν</mi><mn>12</mn></msub></mrow></math></span> band of <sup>13</sup>CD<sub>2</sub>NOH of this work. The rms deviation of the GSCD fit was 0.00040 cm<sup>−1</sup><span>. Additionally, all 3 rotational constants and 5 quartic centrifugal distortion terms of the ground state and 3 rotational constants of the </span><span><math><mrow><msub><mi>v</mi><mn>12</mn></msub></mrow></math></span> = 1 state of <sup>13</sup>CD<sub>2</sub><span>NOH were computed from theoretical anharmonic calculations at two different levels of theory, B3LYP and MP2 with the cc-pVTZ basis set, for comparison with the experimental results. Close agreement was found for the calculated and experimental rovibrational constants of </span><sup>13</sup>CD<sub>2</sub>NOH for both ground and <span><math><mrow><msub><mi>v</mi><mn>12</mn></msub></mrow></math></span> = 1 states. The vibrational anharmonic frequencies of the 12 fundamental bands of <sup>13</sup>CD<sub>2</sub>NOH in the 280–4000 cm<sup>−1</sup> region, and their IR band intensities were also calculated using B3LYP and MP2 with the cc-pVTZ basis set, and they were compared with the respective experimental data. Finally, the ground state rotational constants and the band center of the <span><math><mrow><msub><mi>ν</mi><mn>12</mn></msub></mrow></math>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111885"},"PeriodicalIF":1.4,"publicationDate":"2024-01-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139501513","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-06DOI: 10.1016/j.jms.2024.111874
Kaylee X. Shook, Lindsey M. McDivitt, Caleb D. Shiery, Josiah R. Bailey, Timothy J. McMahon, Robert A. Grimminger, Ryan G. Bird
In this study, the microwave spectra of 2-, 3-, and 4-picolyamine were recorded in a pulsed supersonic jet. With the aid of Natural Bond Orbital analysis, NCIplot, and Multiwfn, the structural effects of substitution were explored and then quantified by comparing semi-experimental geometries. The conformational landscape of each molecule is dominated by Van der Waals interactions between the amino group and the pyridine ring. Spectra of 2H, 13C, and 15N were also collected and analyzed.
{"title":"Coulombic or electrostatic: Determination of the effects of substitution on the structures of 2-, 3-, and 4-picolylamine using Fourier transform microwave spectroscopy","authors":"Kaylee X. Shook, Lindsey M. McDivitt, Caleb D. Shiery, Josiah R. Bailey, Timothy J. McMahon, Robert A. Grimminger, Ryan G. Bird","doi":"10.1016/j.jms.2024.111874","DOIUrl":"10.1016/j.jms.2024.111874","url":null,"abstract":"<div><p>In this study, the microwave spectra of 2-, 3-, and 4-picolyamine were recorded in a pulsed supersonic jet. With the aid of Natural Bond Orbital analysis, NCIplot, and Multiwfn, the structural effects of substitution were explored and then quantified by comparing semi-experimental geometries. The conformational landscape of each molecule is dominated by Van der Waals interactions between the amino group and the pyridine ring. Spectra of <sup>2</sup>H, <sup>13</sup>C, and <sup>1</sup><sup>5</sup>N were also collected and analyzed.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111874"},"PeriodicalIF":1.4,"publicationDate":"2024-01-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139396291","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-01DOI: 10.1016/j.jms.2023.111873
Yujie Zhao , Yali Tian , Xiaohu He , Ting Gong , Xiaocong Sun , Guqing Guo , Xuanbing Qiu , Xiang Yuan , Jinjun Liu , Lunhua Deng , Chuanliang Li
The four lowest Ω substates (X2Π3/2,g, X2Π1/2,g, A2Π3/2,u and A2Π1/2,u) of the cation have been studied by high-precision ab initio calculations in comparison with experimental high-resolution absorption spectra. The potential energy curves were calculated using the multi-reference configuration interaction (MRCI) method and Dirac method, respectively. Rovibrational levels of these electronic states were derived by solving the radial Schrödinger rovibrational equation. Molecular constants were obtained in fitting energy levels to a spectroscopic model. Using the fit spectroscopic constants and newly calculated transition dipole moment matrix elements, line strengths of vibronic bands in the A2Π3/2,u- X2Π3/2,g system, as well as Einstein A coefficients for 45 of these bands with ν′ = 11–19 and ν′′ = 1–5, have been derived. The Einstein A coefficients were used to compute radiative lifetimes of the ν′ = 11–19 vibrational levels of the A2Π3/2,u state. Enhancement factors for detecting the variation of the fine-structure constant (α) and the proton-to-electron mass ratio(µ) using transitions between nearly degenerate rovibronic levels of these low-lying states have been calculated.
通过高精度 ab initio 计算与实验高分辨率吸收光谱的对比,研究了 I2+ 阳离子的四个最低 Ω 子态(X2Π3/2,g、X2Π1/2,g、A2Π3/2,u 和 A2Π1/2,u)。势能曲线分别采用多参考构型相互作用(MRCI)方法和狄拉克方法计算得出。这些电子态的振动水平是通过求解径向薛定谔振动方程得到的。分子常数是通过能级与光谱模型的拟合得到的。利用拟合的光谱常数和新计算的过渡偶极矩矩阵元素,得出了 A2Π3/2,u-X2Π3/2,g系统中振动带的线强度,以及其中ν′=11-19和ν′=1-5的45条带的爱因斯坦A系数。爱因斯坦 A 系数被用来计算 A2Π3/2,u态的ν′=11-19振动级的辐射寿命。计算出了利用这些低洼态的近乎退化的振动级之间的跃迁来探测精细结构常数(α)和质子-电子质量比(µ)变化的增强因子。
{"title":"A spectroscopic investigation of the lowest electronic states of the I2+ cation as a candidate for detecting the time variation of fundamental constants","authors":"Yujie Zhao , Yali Tian , Xiaohu He , Ting Gong , Xiaocong Sun , Guqing Guo , Xuanbing Qiu , Xiang Yuan , Jinjun Liu , Lunhua Deng , Chuanliang Li","doi":"10.1016/j.jms.2023.111873","DOIUrl":"https://doi.org/10.1016/j.jms.2023.111873","url":null,"abstract":"<div><p>The four lowest Ω substates (<em>X</em><sup>2</sup>Π<sub>3/2,g</sub>, <em>X</em><sup>2</sup>Π<sub>1/2,g</sub>, <em>A</em><sup>2</sup>Π<sub>3/2,u</sub> and <em>A</em><sup>2</sup>Π<sub>1/2,u</sub>) of the <span><math><mrow><msubsup><mtext>I</mtext><mn>2</mn><mo>+</mo></msubsup></mrow></math></span> cation have been studied by high-precision <em>ab initio</em> calculations in comparison with experimental high-resolution absorption spectra. The potential energy curves were calculated using the multi-reference configuration interaction (MRCI) method and Dirac method, respectively. Rovibrational levels of these electronic states were derived by solving the radial Schrödinger rovibrational equation. Molecular constants were obtained in fitting energy levels to a spectroscopic model. Using the fit spectroscopic constants and newly calculated transition dipole moment matrix elements, line strengths of vibronic bands in the <em>A</em><sup>2</sup>Π<sub>3/2,u</sub>- <em>X</em><sup>2</sup>Π<sub>3/2,g</sub> system, as well as Einstein <em>A</em> coefficients for 45 of these bands with <em>ν′</em> = 11–19 and <em>ν′′</em> = 1–5, have been derived. The Einstein <em>A</em> coefficients were used to compute radiative lifetimes of the <em>ν′</em> = 11–19 vibrational levels of the <em>A</em><sup>2</sup>Π<sub>3/2,u</sub> state. Enhancement factors for detecting the variation of the fine-structure constant (<em>α</em>) and the proton-to-electron mass ratio(<em>µ</em>) using transitions between nearly degenerate rovibronic levels of these low-lying states have been calculated.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"399 ","pages":"Article 111873"},"PeriodicalIF":1.4,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139100532","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-01-01DOI: 10.1016/j.jms.2023.111872
Josie R. Glenn , J.E. Isert , Jacob D. Bethke , Gamil A. Guirgis , G.S. Grubbs II
The microwave rotational spectrum of 1-ethylsilacyclopentane has been observed using chirped-pulse, Fourier transform microwave spectroscopy and has been reported for the first time. The lowest three energetic conformers were observed and fit to a Watson S semirigid Hamiltonian to within experimental accuracy. The quantum chemical calculations are all within ≈1% of the determined rotational constants, providing confidence that they are accurate representations of the experimental structure. Centrifugal distortion terms DJK and DK, although seemingly large, have been determined to be physically meaningful as no apparent evidence such as splittings in the spectrum or transition broadening was observed. A second moment analysis was undertaken and compared to similar silacyclopentanes, but it is not clear if this species follows previously determined trends.
{"title":"The microwave spectrum of the low energy conformers of 1-ethylsilacyclopentane","authors":"Josie R. Glenn , J.E. Isert , Jacob D. Bethke , Gamil A. Guirgis , G.S. Grubbs II","doi":"10.1016/j.jms.2023.111872","DOIUrl":"10.1016/j.jms.2023.111872","url":null,"abstract":"<div><p>The microwave rotational spectrum of 1-ethylsilacyclopentane has been observed using chirped-pulse, Fourier transform microwave spectroscopy and has been reported for the first time. The lowest three energetic conformers were observed and fit to a Watson S semirigid Hamiltonian to within experimental accuracy. The quantum chemical calculations are all within ≈1% of the determined rotational constants, providing confidence that they are accurate representations of the experimental structure. Centrifugal distortion terms <em>D<sub>JK</sub></em> and <em>D<sub>K</sub></em>, although seemingly large, have been determined to be physically meaningful as no apparent evidence such as splittings in the spectrum or transition broadening was observed. A second moment analysis was undertaken and compared to similar silacyclopentanes, but it is not clear if this species follows previously determined trends.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"399 ","pages":"Article 111872"},"PeriodicalIF":1.4,"publicationDate":"2024-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139021346","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-12-20DOI: 10.1016/j.jms.2023.111872
Josie R. Glenn, J.E. Isert, Jacob D. Bethke, Gamil A. Guirgis, G.S. Grubbs II
The microwave rotational spectrum of 1-ethylsilacyclopentane has been observed using chirped-pulse, Fourier transform microwave spectroscopy and has been reported for the first time. The lowest three energetic conformers were observed and fit to a Watson S semirigid Hamiltonian to within experimental accuracy. The quantum chemical calculations are all within ≈1% of the determined rotational constants, providing confidence that they are accurate representations of the experimental structure. Centrifugal distortion terms DJK and DK, although seemingly large, have been determined to be physically meaningful as no apparent evidence such as splittings in the spectrum or transition broadening was observed. A second moment analysis was undertaken and compared to similar silacyclopentanes, but it is not clear if this species follows previously determined trends.
{"title":"The microwave spectrum of the low energy conformers of 1-ethylsilacyclopentane","authors":"Josie R. Glenn, J.E. Isert, Jacob D. Bethke, Gamil A. Guirgis, G.S. Grubbs II","doi":"10.1016/j.jms.2023.111872","DOIUrl":"https://doi.org/10.1016/j.jms.2023.111872","url":null,"abstract":"<p>The microwave rotational spectrum of 1-ethylsilacyclopentane has been observed using chirped-pulse, Fourier transform microwave spectroscopy and has been reported for the first time. The lowest three energetic conformers were observed and fit to a Watson S semirigid Hamiltonian to within experimental accuracy. The quantum chemical calculations are all within ≈1% of the determined rotational constants, providing confidence that they are accurate representations of the experimental structure. Centrifugal distortion terms <em>D<sub>JK</sub></em> and <em>D<sub>K</sub></em>, although seemingly large, have been determined to be physically meaningful as no apparent evidence such as splittings in the spectrum or transition broadening was observed. A second moment analysis was undertaken and compared to similar silacyclopentanes, but it is not clear if this species follows previously determined trends.</p>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"31 1","pages":""},"PeriodicalIF":1.4,"publicationDate":"2023-12-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139022394","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-12-05DOI: 10.1016/j.jms.2023.111863
V.G. Ushakov , S.A. Balashev , E.S. Medvedev
The potential-energy and quadrupole-moment functions of the H ground electronic state are well known in literature (Komasa et al., 2019; Wolniewicz et al., 1998), and the line list of the vibrational–rotational transitions was calculated (Roueff et al., 2019). In this paper, we analyze the calculated intensities in order to learn how the intensities will change when analytic quadrupole-moment functions fitted to the ab initio and experimental data are used instead of spline-interpolated functions. We found that the use of splines does not deteriorate the intensities and does not lead to nonphysical saturation, as in heavier molecules, owing to the high precision of the ab initio data and the high density of the grid. The accuracy of the calculated intensities is estimated up to high overtones. Extraction of new spectroscopic information from the observational data that supplements the laboratory measurements is performed. The laboratory and observational data do not help increase the quality of the analytic functions. Numerous anomalies resulting from the destructive interference are identified in the calculated line lists, some of them being situated within the recently observed spectral regions, 1.5–. The intensities of these anomalies can be sensitive to the form of the molecular functions as well as to the proton-to-electron mass ratio. In this connection, the similar Le Roy anomalies (Brown and LeRoy, 1973; Le Roy and Vrscay, 1975) also arising due to the destructive interference in the Lyman and Werner systems are discussed.
H2基电子态的势能和四极矩函数在文献中是众所周知的(Komasa et al., 2019;Wolniewicz et al., 1998),并计算了振动-旋转转换的线列表(Roueff et al., 2019)。本文对计算得到的强度进行了分析,以了解当用拟合的解析四极矩函数和实验数据代替样条插值函数时强度的变化情况。我们发现,由于初始数据的高精度和网格的高密度,样条的使用不会降低强度,也不会像在较重的分子中那样导致非物理饱和。计算强度的精度估计到高泛音。从观测数据中提取新的光谱信息,补充实验室测量结果。实验室和观测数据无助于提高分析函数的质量。在计算的谱线表中发现了许多由破坏性干涉引起的异常,其中一些位于最近观测到的1.5-2.5μm光谱区域内。这些异常的强度可以对分子功能的形式以及质子与电子的质量比敏感。在这方面,类似的勒罗伊异常(Brown and LeRoy, 1973;Le Roy和Vrscay, 1975)也讨论了由于Lyman和Werner系统中的破坏性干涉而引起的。
{"title":"Analysis of the calculated and observed X-X ro-vibrational transition intensities in molecular hydrogen","authors":"V.G. Ushakov , S.A. Balashev , E.S. Medvedev","doi":"10.1016/j.jms.2023.111863","DOIUrl":"10.1016/j.jms.2023.111863","url":null,"abstract":"<div><p>The potential-energy and quadrupole-moment functions of the H<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span> ground electronic state are well known in literature (Komasa et al., 2019; Wolniewicz et al., 1998), and the line list of the vibrational–rotational transitions was calculated (Roueff et al., 2019). In this paper, we analyze the calculated intensities in order to learn how the intensities will change when analytic quadrupole-moment functions fitted to the <em>ab initio</em> and experimental data are used instead of spline-interpolated functions. We found that the use of splines does not deteriorate the intensities and does not lead to nonphysical saturation, as in heavier molecules, owing to the high precision of the <em>ab initio</em> data and the high density of the grid. The accuracy of the calculated intensities is estimated up to high overtones. Extraction of new spectroscopic information from the observational data that supplements the laboratory measurements is performed. The laboratory and observational data do not help increase the quality of the analytic functions. Numerous anomalies resulting from the destructive interference are identified in the calculated line lists, some of them being situated within the recently observed spectral regions, 1.5–<span><math><mrow><mn>2</mn><mo>.</mo><mn>5</mn><mspace></mspace><mi>μ</mi><mi>m</mi></mrow></math></span>. The intensities of these anomalies can be sensitive to the form of the molecular functions as well as to the proton-to-electron mass ratio. In this connection, the similar Le Roy anomalies (Brown and LeRoy, 1973; Le Roy and Vrscay, 1975) also arising due to the destructive interference in the Lyman and Werner systems are discussed.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"399 ","pages":"Article 111863"},"PeriodicalIF":1.4,"publicationDate":"2023-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"138529739","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}