2019
DOI: 10.1016/j.asr.2019.07.020
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New techniques for retrieving the [O(3P)], [O3] and [CO2] altitude profiles from dayglow oxygen emissions: Uncertainty analysis by the Monte Carlo method

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Cited by 10 publications
(22 citation statements)
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“…The data incompleteness does not allow to sufficiently describe the radiative quenching in photochemical modelling. Therefore, Yankovsky et al [2] presented an estimation of the Einstein coefficients for emission transitions in the O2 atmospheric, IR atmospheric, and Noxon bands based on values of the Franck-Condon factor from [71]. [62].…”
Section: Emission Transitionsmentioning
confidence: 99%
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“…The data incompleteness does not allow to sufficiently describe the radiative quenching in photochemical modelling. Therefore, Yankovsky et al [2] presented an estimation of the Einstein coefficients for emission transitions in the O2 atmospheric, IR atmospheric, and Noxon bands based on values of the Franck-Condon factor from [71]. [62].…”
Section: Emission Transitionsmentioning
confidence: 99%
“…where v v v -transition energy in cm −1 , q v v -Franck-Condon factor for transition from the level with vibrational number v to the level with vibrational number v", taken from [71]. Results of calculations by (15) for the atmospheric, Noxon, and IR atmospheric bands, respectively, are presented in [2]. The values of the Einstein coefficient for transitions from v = 0-10 to v"= 0-14 in the O 2 atmospheric band [2] allow us to estimate the probability of radiative quenching for levels O 2 (b 1 Σ g + , v = 0-10) ( Figure 7).…”
Section: Details Of Calculation Transitions Referencementioning
confidence: 99%
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“…At lower altitude, the quenching-related decay of O 2 (a 1 ∆ g , v' = 0) is significant because the probability of quenching determines the lifetime of O 2 (a 1 ∆ g , v' = 0), while at higher altitude, the local thermodynamic equilibrium (LTE) is broken because of the presence of constant sources of excited molecular oxygen due to O 2 and O 3 photodissociation. O 2 (a 1 ∆ g ) is formed mainly by photolysis of O 3 in the Hartley band below about 100 km and by energy transfer from O( 1 D) above that altitude [20,22]. The collisional quenching of O 2 (b 1 Σ g ) with N 2 and O 2 also contributes to the production of O 2 (a 1 ∆ g ), especially at 65-85 km.…”
Section: B)mentioning
confidence: 99%