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
Near-Infrared Diode Laser Spectroscopy of the CCO Radical: Molecular Constants for the X̃3Σ−(010) State
✍ Scribed by N. Ohashi; R. Kiryu; S. Okino; M. Fujitake
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 249 KB
- Volume
- 157
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
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} \Sigma^{{ }^{-1}}-\hat{X}(000)^{3} \Sigma^{-} . \tilde{A}(010)^{3} \Sigma^{(-)}-\tilde{X}(010)^{3}) II (b), and (\hat{A}(010)^{3} \Sigma^{1+1}-\dot{X}(010)^{3} I I(b)) bands. These energy differences were analyzed to determine molecular constants for the (\hat{X}(010)) II (b) state in detail. Gi 1993 Academic Press. Inc.
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