We produced aniline cations (–C6H5NH2+) and their dehydro- (H-loss) cations inside helium droplets by electron ionization and observed their mass-selected vibrational spectra in the NH stretching region. We observed vibrational bands at m/q = 93 which were identified as aniline cations. These bands showed only a few cm−1 shifts from the symmetric and anti-symmetric NH stretching bands for the amino (NH2) group in the gas phase. For the H-loss cation at mass m/q = 92, the agreement of the observed NH band frequency with the result of DFT calculations suggests several candidate species, including a seven-membered ring structure, 4-monodehydro azepinylium (–C6NH6+). A new reaction pathway to this cation was discussed by considering large excess energy in the ionization process.
{"title":"Vibrational spectroscopy of aniline cations and their H-loss cations in helium droplets","authors":"Arisa Iguchi , Amandeep Singh , Susumu Kuma , Hajime Tanuma , Toshiyuki Azuma","doi":"10.1016/j.jms.2024.111903","DOIUrl":"10.1016/j.jms.2024.111903","url":null,"abstract":"<div><p>We produced aniline cations (<span><math><mi>c</mi></math></span>–C<sub>6</sub>H<sub>5</sub> <img>NH<sub>2</sub><sup>+</sup>) and their dehydro- (H-loss) cations inside helium droplets by electron ionization and observed their mass-selected vibrational spectra in the N<img>H stretching region. We observed vibrational bands at <em>m/q</em> = 93 which were identified as aniline cations. These bands showed only a few cm<sup>−1</sup> shifts from the symmetric and anti-symmetric N<img>H stretching bands for the amino (<img>NH<sub>2</sub>) group in the gas phase. For the H-loss cation at mass <em>m/q</em> = 92, the agreement of the observed N<img>H band frequency with the result of DFT calculations suggests several candidate species, including a seven-membered ring structure, 4-monodehydro azepinylium (<span><math><mi>c</mi></math></span>–C<sub>6</sub>NH<sub>6</sub><sup>+</sup>). A new reaction pathway to this cation was discussed by considering large excess energy in the ionization process.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"401 ","pages":"Article 111903"},"PeriodicalIF":1.4,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140398430","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 : 2024-03-01Epub Date: 2024-03-15DOI: 10.1016/j.jms.2024.111900
Muhammad Osama Ishtiak , Orfeo Colebatch , Karine Le Bris , Paul J. Godin , Kimberly Strong
Perfluoro-n-propane, perfluorocyclobutane, perfluoro-n-butane, and perfluoro-n-pentane are non-ozone-depleting industrial alternatives to chlorofluorocarbons and hydrochlorofluorocarbons. However, these perfluoroalkanes have significant band strength in the atmospheric window from 800 to 1200 cm−1. Coupled with their millennial-scale atmospheric lifetimes, they can lead to significant long-term global warming. Infrared spectra are required to quantify the climate impacts. This work provides a set of high-temperature infrared absorption cross-sections in the range 298–350 K at 0.1 cm−1 resolution from 515 to 1500 cm−1 for each compound. Our cross-sections generally agree with literature measurements except for perfluoro-n-pentane. We use density functional theory to calculate the absorption cross-sections from 0 to 515 cm−1 using the B3LYP functional and several basis sets. The 6-31G(d,p) basis set provides the best results for linear perfluoroalkanes, while the def2-TZVP basis set provides the best results for cyclic perfluoroalkanes. Using experimental cross-sections, we calculate the radiative efficiency and global warming potential for each compound, utilizing the Pinnock curve from Shine and Myhre (2020) and atmospheric lifetimes from Hodnebrog et al. (2020). These quantities are found to be independent of temperature. The average 100-year global warming potential derived from all cross-sections is 9,610±1,260, 10,800±1,420, 10,100±1,330, and 9,380±1,230 for perfluoro-n-propane, perfluorocyclobutane, perfluoro-n-butane, and perfluoro-n-pentane, respectively. Combining the data in this work with our previous measurements reveals that the global warming potential for perfluoroalkanes with an increasing number of CF bonds depends on the ratio of radiative efficiency to molecular weight.
{"title":"Measurements of infrared absorption cross-sections for n-C3F8, c-C4F8, n-C4F10, and n-C5F12 from 298 to 350 K","authors":"Muhammad Osama Ishtiak , Orfeo Colebatch , Karine Le Bris , Paul J. Godin , Kimberly Strong","doi":"10.1016/j.jms.2024.111900","DOIUrl":"10.1016/j.jms.2024.111900","url":null,"abstract":"<div><p>Perfluoro-n-propane, perfluorocyclobutane, perfluoro-n-butane, and perfluoro-n-pentane are non-ozone-depleting industrial alternatives to chlorofluorocarbons and hydrochlorofluorocarbons. However, these perfluoroalkanes have significant band strength in the atmospheric window from 800 to 1200 cm<sup>−1</sup>. Coupled with their millennial-scale atmospheric lifetimes, they can lead to significant long-term global warming. Infrared spectra are required to quantify the climate impacts. This work provides a set of high-temperature infrared absorption cross-sections in the range 298–350 K at 0.1 cm<sup>−1</sup> resolution from 515 to 1500 cm<sup>−1</sup> for each compound. Our cross-sections generally agree with literature measurements except for perfluoro-n-pentane. We use density functional theory to calculate the absorption cross-sections from 0 to 515 cm<sup>−1</sup> using the B3LYP functional and several basis sets. The 6-31G(d,p) basis set provides the best results for linear perfluoroalkanes, while the def2-TZVP basis set provides the best results for cyclic perfluoroalkanes. Using experimental cross-sections, we calculate the radiative efficiency and global warming potential for each compound, utilizing the Pinnock curve from Shine and Myhre (2020) and atmospheric lifetimes from Hodnebrog et al. (2020). These quantities are found to be independent of temperature. The average 100-year global warming potential derived from all cross-sections is 9,610±1,260, 10,800±1,420, 10,100±1,330, and 9,380±1,230 for perfluoro-n-propane, perfluorocyclobutane, perfluoro-n-butane, and perfluoro-n-pentane, respectively. Combining the data in this work with our previous measurements reveals that the global warming potential for perfluoroalkanes with an increasing number of C<img>F bonds depends on the ratio of radiative efficiency to molecular weight.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"401 ","pages":"Article 111900"},"PeriodicalIF":1.4,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0022285224000274/pdfft?md5=1606f942c2fb317c06570494fb3fba8f&pid=1-s2.0-S0022285224000274-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140154167","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01Epub Date: 2024-01-23DOI: 10.1016/j.jms.2024.111886
Michael C. McCarthy, P. Bryan Changala, P. Brandon Carroll
The rotational spectra of two new silicon-bearing carbon chains, H2C3Si and HSiCCH have been detected by means of Fourier-transform microwave spectroscopy in a supersonic jet source equipped with an electrical discharge. On the basis of measurements between 10 and 42 GHz, precise spectroscopic constants have been determined for both molecules. Along with H29SiCCH and H30SiCCH, which were detected in natural abundance, several other rare isotopic species of HSiCCH were observed using samples enriched in carbon-13 and D. From this isotopic data, a precise semi-experimental equilibrium structure was derived and compared with a re-evaluated semi-experimental equilibrium structure of the parent silylene SiH2; the deuterium isotopic measurements also provide important clues as to the formation pathway of HSiCCH in our discharge. Because other small Si-bearing chains have been detected in the circumstellar envelope of the evolved carbon star IRC+10216, both chains may be of astronomical interest.
{"title":"Rotational detection of the silicon-carbon chains H2C3Si and HSiCCH","authors":"Michael C. McCarthy, P. Bryan Changala, P. Brandon Carroll","doi":"10.1016/j.jms.2024.111886","DOIUrl":"10.1016/j.jms.2024.111886","url":null,"abstract":"<div><p>The rotational spectra of two new silicon-bearing carbon chains, H<sub>2</sub>C<sub>3</sub>Si and HSiCCH have been detected by means of Fourier-transform microwave spectroscopy in a supersonic jet source equipped with an electrical discharge. On the basis of measurements between 10 and 42<!--> <!-->GHz, precise spectroscopic constants have been determined for both molecules. Along with H<sup>29</sup>SiCCH and H<sup>30</sup>SiCCH, which were detected in natural abundance, several other rare isotopic species of HSiCCH were observed using samples enriched in carbon-13 and D. From this isotopic data, a precise semi-experimental equilibrium structure was derived and compared with a re-evaluated semi-experimental equilibrium structure of the parent silylene SiH<sub>2</sub>; the deuterium isotopic measurements also provide important clues as to the formation pathway of HSiCCH in our discharge. Because other small Si-bearing chains have been detected in the circumstellar envelope of the evolved carbon star IRC+10216, both chains may be of astronomical interest.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111886"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139557719","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 : 2024-02-01Epub Date: 2024-02-09DOI: 10.1016/j.jms.2024.111887
Aaron I. Strom , Ibrahim Muddasser , Guntram Rauhut , David T. Anderson
The vibrational dynamics of diborane have been extensively studied both theoretically and experimentally ever since the bridge structure of diborane was established in the 1950s. Numerous infrared and several Raman spectroscopic studies have followed in the ensuing years at ever increasing levels of spectral resolution. In parallel, ab initio computations of the underlying potential energy surface have progressed as well as the methods to calculate the anharmonic vibration dynamics beyond the double harmonic approximation. Nevertheless, even 70 years after the bridge structure of diborane was established, there are still significant discrepancies between experiment and theory for the fundamental vibrational frequencies of diborane. In this work we use parahydrogen (pH2) matrix isolation infrared spectroscopy to characterize six fundamental vibrations of B2H6 and B2D6 and compare them with results from configuration-selective vibrational configuration interaction theory. The calculated frequencies and intensities are in very good agreement with the pH2 matrix isolation spectra, even several combination bands are well reproduced. We believe that the reason discrepancies have existed for so long is related to the large amount of anharmonicity that is associated with the bridge BH stretching modes. However, the calculated frequencies and intensities reported here for the vibrational modes of all three boron isotopologues of B2H6 and B2D6 are within ± 2.00 cm−1 and ± 1.44 cm−1, respectively, of the experimental frequencies and therefore a refined vibrational assignment of diborane has been achieved.
{"title":"Diborane anharmonic vibrational frequencies and Intensities: Experiment and theory","authors":"Aaron I. Strom , Ibrahim Muddasser , Guntram Rauhut , David T. Anderson","doi":"10.1016/j.jms.2024.111887","DOIUrl":"https://doi.org/10.1016/j.jms.2024.111887","url":null,"abstract":"<div><p>The vibrational dynamics of diborane have been extensively studied both theoretically and experimentally ever since the bridge structure of diborane was established in the 1950s. Numerous infrared and several Raman spectroscopic studies have followed in the ensuing years at ever increasing levels of spectral resolution. In parallel, <em>ab initio</em> computations of the underlying potential energy surface have progressed as well as the methods to calculate the anharmonic vibration dynamics beyond the double harmonic approximation. Nevertheless, even 70 years after the bridge structure of diborane was established, there are still significant discrepancies between experiment and theory for the fundamental vibrational frequencies of diborane. In this work we use parahydrogen (pH<sub>2</sub>) matrix isolation infrared spectroscopy to characterize six fundamental vibrations of B<sub>2</sub>H<sub>6</sub> and B<sub>2</sub>D<sub>6</sub> and compare them with results from configuration-selective vibrational configuration interaction theory. The calculated frequencies and intensities are in very good agreement with the pH<sub>2</sub> matrix isolation spectra, even several combination bands are well reproduced. We believe that the reason discrepancies have existed for so long is related to the large amount of anharmonicity that is associated with the bridge BH stretching modes. However, the calculated frequencies and intensities reported here for the vibrational modes of all three boron isotopologues of B<sub>2</sub>H<sub>6</sub> and B<sub>2</sub>D<sub>6</sub> are within ± 2.00 cm<sup>−1</sup> and ± 1.44 cm<sup>−1</sup>, respectively, of the experimental frequencies and therefore a refined vibrational assignment of diborane has been achieved.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111887"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139733136","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 : 2024-02-01Epub 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":"2024-02-01","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}
In this experimental investigation, collision broadening effects on the Q(J)-branch vibration-inversion-rotation spectral lines of ammonia (NH3) within the fundamental asymmetric bending vibrational band in the 6.2 µm mid-IR region are reported. A continuous-wave external-cavity quantum cascade laser coupled with a high-sensitive cavity ring-down spectrometer was employed to selectively probe 10 transitions in high-resolution, including few inversion doublets of gaseous NH3. Pressure-broadening coefficients, ( = He, Ar, N2, O2, zero-air) in cm−1 atm−1, characterizing the collision interaction between NH3 and various external perturbing gases, including helium, argon, nitrogen, oxygen, and zero-air, were determined at room temperature (296 K). Mean collision times and optical collision diameters of each collision partner were explored to gain deeper insight into the perturber-induced collision dynamics. This investigation elucidates the intricate intermolecular interactions and collision phenomena induced by various foreign perturbers with NH3, with potential implications for future spectroscopic and atmospheric research of this polyatomic molecule.
{"title":"Collision-broadening of vibration-inversion-rotation ammonia spectral lines in Q(J)-branch at 6.2 µm by cavity ring-down spectroscopy","authors":"Soumyadipta Chakraborty, Indrayani Patra, Ardhendu Pal, Manik Pradhan","doi":"10.1016/j.jms.2024.111891","DOIUrl":"https://doi.org/10.1016/j.jms.2024.111891","url":null,"abstract":"<div><p>In this experimental investigation, collision broadening effects on the Q(J)-branch vibration-inversion-rotation spectral lines of ammonia (NH<sub>3</sub>) within the fundamental <span><math><msub><mi>ν</mi><mn>4</mn></msub></math></span> asymmetric bending vibrational band in the 6.2 µm mid-IR region are reported. A continuous-wave external-cavity quantum cascade laser coupled with a high-sensitive cavity ring-down spectrometer was employed to selectively probe 10 transitions in high-resolution, including few inversion doublets of gaseous NH<sub>3</sub>. Pressure-broadening coefficients, <span><math><msub><mi>γ</mi><mrow><mi>N</mi><msub><mi>H</mi><mn>3</mn></msub><mo>-</mo><msub><mi>X</mi><mi>i</mi></msub></mrow></msub></math></span> (<span><math><msub><mi>X</mi><mi>i</mi></msub></math></span> = He, Ar, N<sub>2,</sub> O<sub>2,</sub> zero-air) in cm<sup>−1</sup> atm<sup>−1</sup>, characterizing the collision interaction between NH<sub>3</sub> and various external perturbing gases, including helium, argon, nitrogen, oxygen, and zero-air, were determined at room temperature (296 K). Mean collision times and optical collision diameters of each collision partner were explored to gain deeper insight into the perturber-induced collision dynamics. This investigation elucidates the intricate intermolecular interactions and collision phenomena induced by various foreign perturbers with NH<sub>3</sub>, with potential implications for future spectroscopic and atmospheric research of this polyatomic molecule.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111891"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140031070","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 : 2024-02-01Epub Date: 2024-02-12DOI: 10.1016/j.jms.2024.111888
H. Zarringhalam , D.W. Tokaryk , A.G. Adam , C. Linton
Laser Induced Fluorescence (LIF) has been used to study the spectroscopy of ruthenium monofluoride (RuF) in the UNB laser-ablation molecular-jet apparatus. High-resolution spectra of three band systems have been obtained, with a linewidth (FWHM) of ∼0.004 cm−1, in the near infrared (NIR), green and blue regions at ∼ 760 nm, 548 nm and 450 nm respectively. Electronic states have been assigned based on observation of first lines in the R and P branches and the excited states are labelled A, B and C in increasing energy order. Three transitions have been assigned to the green system as spin–orbit components, B4Γ5.5 – X4Φ4.5 and B4Γ4.5 – X4Φ3.5 of the (0,0) band, and B4Γ5.5 – X4Φ4.5 of the (1,1) band of the B – X system. The single NIR and blue bands were assigned as A4Δ3.5 - X4Φ4.5 (0,0) and C4Δ3.5 - X4Φ4.5 (0,0) respectively. Rotational structure of four individual isotopologues 96RuF, 100RuF, 102RuF and 104RuF was well resolved and used to examine the rotational and vibrational isotope effects. The rotational lines were doubled by hyperfine structure due to the nuclear spin I = ½ of fluorine. The hyperfine structure due to the nuclear spin I = 5/2 of 99Ru and 101Ru was not resolved resulting in weak broadened 99RuF and 101RuF lines that were overlapped by the stronger lines of the other isotopologues and could only be assigned in the C4Δ3.5 - X4Φ4.5 (0,0) band. The fluorine hyperfine structure was used to estimate the fraction of F 2sσ and 2pπ in the Ru-centered σ and π molecular orbitals.
在 UNB 激光烧蚀分子喷射装置中,利用激光诱导荧光(LIF)研究了单氟化钌(RuF)的光谱。在近红外(NIR)、绿光和蓝光区域,分别在 ∼ 760 nm、548 nm 和 450 nm 处获得了线宽(FWHM)为 ∼0.004 cm-1 的三个波段系统的高分辨率光谱。根据对 R 支和 P 支中第一条线的观察,对电子状态进行了分配,激发态按能量递增顺序标为 A、B 和 C。绿色系统的三个跃迁被指定为自旋轨道成分,即(0,0)波段的 B4Γ5.5 - X4Φ4.5 和 B4Γ4.5 - X4Φ3.5,以及 B - X 系统(1,1)波段的 B4Γ5.5 - X4Φ4.5。单一的近红外波段和蓝光波段分别被命名为 A4Δ3.5 - X4Φ4.5 (0,0) 和 C4Δ3.5 - X4Φ4.5 (0,0)。对四种同素异形体 96RuF、100RuF、102RuF 和 104RuF 的旋转结构进行了很好的解析,并用于研究旋转和振动同位素效应。由于氟的核自旋 I = ½ ,超正弦结构使旋转线加倍。由于 99Ru 和 101Ru 的核自旋 I = 5/2 所产生的超正弦结构未被解析,导致 99RuF 和 101RuF 的线变弱变宽,与其他同位素的较强线重叠,只能归属于 C4Δ3.5 - X4Φ4.5 (0,0) 波段。氟超频结构用于估算 F 2sσ 和 2pπ 在以 Ru 为中心的 σ 和 π 分子轨道中的比例。
{"title":"Rotational and hyperfine structure in the A4Δ – X4Φ, B4Γ – X4Φ and C4Δ – X4Φ transitions of ruthenium monofluoride (RuF)","authors":"H. Zarringhalam , D.W. Tokaryk , A.G. Adam , C. Linton","doi":"10.1016/j.jms.2024.111888","DOIUrl":"10.1016/j.jms.2024.111888","url":null,"abstract":"<div><p>Laser Induced Fluorescence (LIF) has been used to study the spectroscopy of ruthenium monofluoride (RuF) in the UNB laser-ablation molecular-jet apparatus. High-resolution spectra of three band systems have been obtained, with a linewidth (FWHM) of ∼0.004 cm<sup>−1</sup>, in the near infrared (NIR), green and blue regions at ∼ 760 nm, 548 nm and 450 nm respectively. Electronic states have been assigned based on observation of first lines in the R and P branches and the excited states are labelled A, B and C in increasing energy order. Three transitions have been assigned to the green system as spin–orbit components, B<sup>4</sup>Γ<sub>5.5</sub> – X<sup>4</sup>Φ<sub>4.5</sub> and B<sup>4</sup>Γ<sub>4.5</sub> – X<sup>4</sup>Φ<sub>3.5</sub> of the (0,0) band, and B<sup>4</sup>Γ<sub>5.5</sub> – X<sup>4</sup>Φ<sub>4.5</sub> of the (1,1) band of the B – X system. The single NIR and blue bands were assigned as A<sup>4</sup>Δ<sub>3.5</sub> - X<sup>4</sup>Φ<sub>4.5</sub> (0,0) and C<sup>4</sup>Δ<sub>3.5</sub> - X<sup>4</sup>Φ<sub>4.5</sub> (0,0) respectively. Rotational structure of four individual isotopologues <sup>96</sup>RuF, <sup>100</sup>RuF, <sup>102</sup>RuF and <sup>104</sup>RuF was well resolved and used to examine the rotational and vibrational isotope effects. The rotational lines were doubled by hyperfine structure due to the nuclear spin I = ½ of fluorine. The hyperfine structure due to the nuclear spin I = 5/2 of <sup>99</sup>Ru and <sup>101</sup>Ru was not resolved resulting in weak broadened <sup>99</sup>RuF and <sup>101</sup>RuF lines that were overlapped by the stronger lines of the other isotopologues and could only be assigned in the C<sup>4</sup>Δ<sub>3.5</sub> - X<sup>4</sup>Φ<sub>4.5</sub> (0,0) band. The fluorine hyperfine structure was used to estimate the fraction of F 2sσ and 2pπ in the Ru-centered σ and π molecular orbitals.</p></div>","PeriodicalId":16367,"journal":{"name":"Journal of Molecular Spectroscopy","volume":"400 ","pages":"Article 111888"},"PeriodicalIF":1.4,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139890893","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 : 2024-02-01Epub Date: 2023-12-13DOI: 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 : 2024-02-01Epub 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":"2024-02-01","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 : 2024-02-01Epub Date: 2024-02-10DOI: 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}