Abstract

Atmospheric emissions of atomic and molecular oxygen have been observed since the middle of 19th century. In the last decades, it has been shown that emissions of excited oxygen atom O(1D) and molecular oxygen in electronically–vibrationally excited states O2(b1Σ+g, v) and O2(a1Δg, v) are related by a unified photochemical mechanism in the mesosphere and lower thermosphere (MLT). The current paper consists of two parts: a review of studies related to the development of the model of ozone and molecular oxygen photodissociation in the daytime MLT and new results. In particular, the paper includes a detailed description of formation mechanism for excited oxygen components in the daytime MLT and presents comparison of widely used photochemical models. The paper also demonstrates new results such as new suggestions about possible products for collisional reactions of electronically–vibrationally excited oxygen molecules with atomic oxygen and new estimations of O2(b1Σ+g, v = 0–10) radiative lifetimes which are necessary for solving inverse problems in the lower thermosphere. Moreover, special attention is given to the “Barth’s mechanism” in order to demonstrate that for different sets of fitting coefficients its contribution to O2(b1Σ+g, v) and O2(a1Δg, v) population is neglectable in daytime conditions. In addition to the review and new results, possible applications of the daytime oxygen emissions are presented, e.g., the altitude profiles O(3P), O3 and CO2 can be retrieved by solving inverse photochemical problems when emissions from electronically vibrationally excited states of O2 molecule are used as proxies.

Highlights

  • The dayglow and nightglow are dominated by two powerful bands of molecular oxygen, having the names: O2 IR atmospheric (0–0) band with a center at 1.27 μm and O2 atmospheric (0–0) band with a center at 0.762 μm

  • It has been shown that emissions of excited oxygen atom O(1 D)

  • Photolysis of oxygen molecules leads to formation of excited oxygen atoms O(1 D) due to absorption of solar radiation in the Schumann–Runge continuum, which dominates at altitudes above 90 km, and in the H Lyman-α line whose contribution is in the altitude range of 70–90 km

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Summary

Introduction

The dayglow and nightglow are dominated by two powerful bands of molecular oxygen, having the names: O2 IR atmospheric (0–0) band with a center at 1.27 μm and O2 atmospheric (0–0) band with a center at 0.762 μm. In 1986, based on results of multi-rocket ETON (Energy Transfer in the Oxygen Nightglow) experiment, a full-featured model of oxygen emissions at nighttime conditions was designed [15,16,17]. Note that emission bands of an oxygen molecule with much higher levels of vibrational excitation O2 (b1 Σ+ g , v0 = 0–15) are observed in the atmospheric glow [25]. E.g., laboratory experiments from the mid 1970s to the present show that energy transfer as a result of O2 and O3 photolysis carried out with participation of electronically–vibrationally excited levels of oxygen molecule. It becomes more clear when considering the mechanism of heating the.

Formation of Excited Oxygen Components in the Daytime MLT
Block-scheme
O3 Photodissociation and Its Products
Energy
Emission Transitions
Kinetics
Solid orange vertical
Forward Problem
13. Daily altitude profilesof ofO
Inverse Problem
Conclusions
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