1996
DOI: 10.1051/aas:1996173
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Einstein A-coefficients for vib-rotational transitions in CO

Abstract: Abstract. -Einstein A-coefficients for vib-rotational transitions in CO isotopomers, for vibrational quantum number v up to 20, rotational quantum number J up to 140, and ∆v up to 4, are calculated. The change in J is governed by the selection rules ∆J = ±1. These coefficients play an important role in astronomy, as CO is the most abundant molecule after H2, and has been observed in almost all the astronomical objects.

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Cited by 60 publications
(63 citation statements)
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“…Models were also considered that allowed the vibrational levels to fall out of thermal equilibrium while retaining thermal populations for the rotational levels. This is physically plausible, since pure rotational lifetimes are typically 10 4 -10 5 longer than their vibrational-rotational counterparts (Chandra, Maheshwari, & Sharma 1996). Under such conditions, the widths of the band heads are sensitive to the rotational temperature, while their relative intensities are determined primarily by the populations of the vibrational levels.…”
Section: Co Characteristicsmentioning
confidence: 98%
“…Models were also considered that allowed the vibrational levels to fall out of thermal equilibrium while retaining thermal populations for the rotational levels. This is physically plausible, since pure rotational lifetimes are typically 10 4 -10 5 longer than their vibrational-rotational counterparts (Chandra, Maheshwari, & Sharma 1996). Under such conditions, the widths of the band heads are sensitive to the rotational temperature, while their relative intensities are determined primarily by the populations of the vibrational levels.…”
Section: Co Characteristicsmentioning
confidence: 98%
“…B.2 and B.3). The transition frequencies, Einstein A coefficients, statistical weights, and energies of the upper levels are taken from Chandra et al (1996). We approximate the emitting region by a rectangle with the same width as the slit and length equal to the diameter of the emitting region of the CO (2 × 50 AU, Goto et al 2012): Ω = 0.…”
Section: Population Diagramsmentioning
confidence: 99%
“…The optical depth is given by the absorption coefficient per CO molecule × the CO column density (i.e., N(r) because of the thin disc). Our model takes into account up to J = 100 rotational levels in local thermal equilibrium (LTE) for the two transitions, where the CO energy levels and the Einstein coefficients are taken from Farrenq et al (1991) and from Chandra et al (1996), respectively. The disc is split into radial and azimuthal cells.…”
Section: Co Bandhead Modellingmentioning
confidence: 99%