Abstract:The fluorescence excitation (FE) spectrum for the Ã2A2 ↔ X̃2B1 transition of OClO cooled in supersonic jet
expansions has been obtained for the first time from the origin band at 476 nm up to 355 nm. Despite rapid
predissociation of the excited OClO molecules, the fluorescence emission is strong enough to give the FE
spectrum with a high signal-to-noise ratio. The present FE spectrum shows the much lower rotational
temperature and hence better state resolution than seen in previously reported spectra, demonstr… Show more
“…Irradiation at 440 nm results in the formation of FeϩD 2 . 1,2 T 0 ϭ9530(180) gas PE 3 T 0 ϭ11497(10) gas b -ã 465-1049 nm AB 1,3,27,44 LMR 21 LF 33,38,40,42,43 DL [47][48][49][50] Vib. sym.…”
Section: Fedmentioning
confidence: 99%
“…͑0,14,0͒ϭ4.6͑1͒ s LF 9,39 ͑0,16,0͒ϭ1.3͑3͒ s LF 11 3.8͑3͒ s LF 39 B 010 ϭ8.59(4) DL 47 C 2v Structure: AB 3,29,31 T 0 ϭ3147(5) gas b -ã 465-1049 nm AB 1,3,27,28,44 LMR 21,26,30 PE 23,24 LF 32,38,40,42,43,45 SEP 32,34 DL[47][48][49][50] …”
A summary is presented of recently published, critically evaluated experimental vibrational and electronic energy level data for approximately 1700 neutral and ionic transient molecules and high temperature species possessing from three to sixteen atoms. Although the emphasis is on species with lifetimes too short for study using conventional sampling techniques, there has been selective extension of the compilation to include data for isolated molecules of inorganic species such as the heavy-metal oxides, which are important in a wide variety of industrial chemical systems. Radiative lifetimes and the principal rotational constants are included. Observations in the gas phase, in molecular beams, and in rare-gas and diatomic molecule matrices are evaluated, and several thousand references are cited. The types of measurement surveyed include conventional and laser-based absorption and emission techniques, laser absorption with mass analysis, and photoelectron spectroscopy.
“…Irradiation at 440 nm results in the formation of FeϩD 2 . 1,2 T 0 ϭ9530(180) gas PE 3 T 0 ϭ11497(10) gas b -ã 465-1049 nm AB 1,3,27,44 LMR 21 LF 33,38,40,42,43 DL [47][48][49][50] Vib. sym.…”
Section: Fedmentioning
confidence: 99%
“…͑0,14,0͒ϭ4.6͑1͒ s LF 9,39 ͑0,16,0͒ϭ1.3͑3͒ s LF 11 3.8͑3͒ s LF 39 B 010 ϭ8.59(4) DL 47 C 2v Structure: AB 3,29,31 T 0 ϭ3147(5) gas b -ã 465-1049 nm AB 1,3,27,28,44 LMR 21,26,30 PE 23,24 LF 32,38,40,42,43,45 SEP 32,34 DL[47][48][49][50] …”
A summary is presented of recently published, critically evaluated experimental vibrational and electronic energy level data for approximately 1700 neutral and ionic transient molecules and high temperature species possessing from three to sixteen atoms. Although the emphasis is on species with lifetimes too short for study using conventional sampling techniques, there has been selective extension of the compilation to include data for isolated molecules of inorganic species such as the heavy-metal oxides, which are important in a wide variety of industrial chemical systems. Radiative lifetimes and the principal rotational constants are included. Observations in the gas phase, in molecular beams, and in rare-gas and diatomic molecule matrices are evaluated, and several thousand references are cited. The types of measurement surveyed include conventional and laser-based absorption and emission techniques, laser absorption with mass analysis, and photoelectron spectroscopy.
“…But, no vibrational level shows the unusual isotopic effect at the higher energies than those covered in this work. 12 Many examples of the isotope effect in the decay rates of the electronically excited states have been reported. 19 Most of the cases are for the H/D isotopes and have been explained in terms of the more rapid tunneling of H atoms through the barrier than D atoms.…”
Section: Resultsmentioning
confidence: 99%
“…12 In short, the OClO mixture in He, kept at the pressure of 1 atm, was expanded through a 0.5 mmdiameter nozzle, which was driven with a homemade driver. The visible wavelengths spanning 480 to 400 nm were directly generated with a pulsed dye laser pumped with a Q-switched Nd:YAG laser.…”
The fluorescence intensity ratios of O37ClO/O35ClO excited to the à 2A2 state have been found to be much larger than that expected from the 37Cl/35Cl natural abundance ratio for several low-energy vibrational levels. For instance, the O37ClO/O35ClO ratios are 1.67 and >10 for the (0,0,0) and (1,1,0) bands, respectively, which are 5 and 30 times larger than those expected from the natural abundance ratio. These unusual isotope effects are observed in a narrow energy region within ∼1000 cm−1 above the electronic origin. It is likely that the isotopomer-selective, near-resonant spin-orbit coupling of the low-energy vibrational levels of the 2A2 state with those of the 2A1 state, which provides a decay channel for the 2A2 state via spin-orbit coupling, is responsible for the unusual isotope effect.
The time-correlation function formalism has been used to calculate resonance Raman cross sections, excitation profiles, and electronic absorption spectra of the OClO molecule in the gas-phase and in different solvents like cyclohexane, chloroform, and water. The multidimensional time domain integrals that arise in these calculations have been evaluated for the case in which an X 2 B 1 -Ã 2 A 1 electronic transition takes place between displaced-distorted-rotated harmonic potential energy surfaces. Ab initio calculations have been performed to provide the spectroscopic constants required for the evaluation of these integrals. The calculated absorption spectra and resonance Raman cross sections have been compared with the experimental results.
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