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AGU: Journal of Geophysical Research, Atmospheres

 

Keywords

  • airglow molecular nitrogen
  • thermosphere

Index Terms

  • Atmospheric Composition and Structure: Airglow and aurora
  • Atmospheric Processes: Radiative processes
  • Atmospheric Composition and Structure: Thermosphere: energy deposition
Abstract
Cited By (0)
 

Abstract

Analysis of terrestrial thermospheric N2c41Σu+(0) ∼b1Σu+(1) −X1Σg+dayglow emission observed by the Far Ultraviolet Spectroscopic Explorer

Xianming Liu

Planetary and Space Science Division, Space Environment Technologies, Pasadena, California, USA

Alan N. Heays

Research School of Physical Sciences and Engineering, Australian National University, Canberra, ACT, Australia

Donald E. Shemansky

Planetary and Space Science Division, Space Environment Technologies, Pasadena, California, USA

Brenton R. Lewis

Research School of Physical Sciences and Engineering, Australian National University, Canberra, ACT, Australia

Paul D. Feldman

Department of Physics and Astronomy, Johns Hopkins University, Baltimore, Maryland, USA

Terrestrial thermospheric dayglow emission from the coupled and overlapping c4 1Σ u +(0) and b1Σ u +(1) levels of molecular nitrogen, observed by the Far Ultraviolet Spectroscopic Explorer, is analyzed with the aid of a coupled channels quantum mechanical model of N2 spectroscopy and predissociation dynamics. Model emission spectra for the mixed c4 1Σ u +(0) ∼ b1Σ u +(1) − X 1Σ g +(v i = 2, 6–9) transitions, calculated for the case of excitation by photoelectron impact, are in excellent agreement with the observations. While the principal excitation mechanism for N2 in the thermosphere is photoelectron impact, evidence is also found in other transitions of resonant fluorescence, induced by lines in the solar atomic hydrogen Lyman series, atomic oxygen transitions, and other N2 bands. The observed emission rate of the c4 1Σ u +(0) ∼ b1Σ u +(1) − X 1Σ g +(0) band is ∼1% of that inferred from the emission rates to X 1Σ g +(v i > 2) levels. A qualitative explanation is given for the drastically reduced intensity and band shape distortion observed in the c4 1Σ u +(0) − X 1Σ g +(0) emission band. Estimates of the total electron excitation rates for the nominal b1Σ u +(1) and c4 1Σ u +(0) levels are determined from the spectrum by extrapolating the model through regions containing unmeasured and/or resonantly absorbed bands.

Received 12 May 2008; accepted 2 February 2009; published 10 April 2009.

Citation: Liu, X., A. N. Heays, D. E. Shemansky, B. R. Lewis, and P. D. Feldman (2009), Analysis of terrestrial thermospheric N2c41Σu+(0) ∼b1Σu+(1) −X1Σg+dayglow emission observed by the Far Ultraviolet Spectroscopic Explorer, J. Geophys. Res., 114, D07304, doi:10.1029/2008JD010403.

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