O<sub>2</sub> (<i>c</i>¹Σ<sub><i>u</i></sub><sup>−</sup> → <i>X</i>³Σ<sub><i>g</i></sub><sup>−</sup>) emission in the terrestrial nightglow

T. G. Slanger, D. L. Huestis

Journal of Geophysical Research Atmospheres · 1981 · 76 citations · 21 references

Concepts

Abstract

Synthetic spectra have been calculated incorporating three O 2 emission systems, A ³Σ u + → X ³Σ g − , A′ ³Δ u → a ¹Δ g , and c ¹Σ u − → X ³Σ g − , and matched to the 3100‐ to 4500‐Å nightglow spectrum of Broadfoot and Kendall (1968). The synthesis necessitated the inclusion of the c ¹Σ u − → X ³Σ g − system, which has never been previously identified in the airglow, although it is a dominant system in the Venusian nightglow. The emissions from the extremely metastable A′ ³Δ u and c ¹Σ u − states account for half the radiation in the 3100‐ to 4500‐Å region, from which it may be deduced that the mesospheric concentrations of O 2 ( A′ ³Δ u ) and O 2 ( c ¹Σ u − ) are much higher than that of O 2 ( A ³Σ u + ). The vibrational distributions are quite unrelaxed for all three states.

References

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