Vib-rotational energy differences between the \(\dot{X}(010)^{3} \Pi(b)\) and \(\dot{X}(000)^{3} \Sigma^{-}\)states, and purerotational energy differences in the \(\bar{X}(010)^{3} \Pi(b)\) state of the CCO radical, were obtained from near-infrared absorption spectral data of the \(\tilde{A}(010)^{3
Near-infrared diode laser spectroscopy of the CCO radical in the Ã3Πi(000)-X̃3Σ−(000) band
✍ Scribed by Masaharu Fujitake; Ryusuke Kiryu; Nobukimi Ohashi
- Publisher
- Elsevier Science
- Year
- 1992
- Tongue
- English
- Weight
- 605 KB
- Volume
- 154
- Category
- Article
- ISSN
- 0022-2852
No coin nor oath required. For personal study only.
📜 SIMILAR VOLUMES
The A ˜(010) 3 ⌬-X ˜(010) 3 ⌸(b) band spectrum of the CCO radical has been studied in the region from 11,808 to 11,919 cm Ϫ1 by near-infrared diode-laser spectroscopy. A least-squares fit has been made using only part of the observed A ˜(010) 3 ⌬-X ˜(010) 3 ⌸(b) band transitions to obtain molecular
The forbidden \(\dot{A}(010)^{2} \Sigma^{(+)},{ }^{2} \Sigma^{(-)}-\dot{X}(000)^{2} \Sigma^{+}\)parallel bands of \(\mathrm{CaOH}\), which gain transition strength through vibronic mixing between different electronic states, have been observed via laserinduced fluorescence. The fundamental bending f
The rotationally resolved infrared spectrum of the v 3 band of the long-lived a31-I u electronic state of C 3 has been observed between 1428 and 1473 cm-~ using a tunable diode laser spectrometer. Metastable C 3 was produced in a discharge through a flowing mixture of acetylene and helium. The obser
The \(\dot{A}(010)^{3} \Sigma^{(-)}-\dot{X}(000)^{3} \Sigma^{-}, \dot{A}(010)^{3} \Sigma^{(-)}-\dot{X}(010)^{3} \Pi(b)\) and \(\dot{A}(010)^{3} \Sigma^{(+)}-\dot{X}(010)^{3} \Pi(b)\) subbands in the \(\dot{A}^{3} \Pi_{i}-\dot{X}^{3} \Sigma^{-}\)system of the \(\mathrm{CCO}\) radical have been reinve