TY - JOUR
T1 - Analysis of terrestrial thermospheric N2 c4′; 1Σu+(0) ∼ b′ 1Σu+(1) - X 1Σ g+ dayglow emission observed by the far ultraviolet spectroscopic explorer
AU - Liu, Xianming
AU - Heays, Alan N.
AU - Shemansky, Donald E.
AU - Lewis, Brenton R.
AU - Feldman, Paul D.
PY - 2009/4/16
Y1 - 2009/4/16
N2 - Terrestrial thermospheric dayglow emission from the coupled and overlapping c4′ 1Σu+-(0) and b′ 1Σu+(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′ 1Σu1(0) ∼ b′ 1Σu+(1) - X1 Σg+ (vi = 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 N 2 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′ 1Σu1(0) ∼ b′ 1Σu+(1) - X 1Σ g+(0) band is ∼1% of that inferred from the emission rates to X 1Σg+(vi > 2) levels. A qualitative explanation is given for the drastically reduced intensity and band shape distortion observed in the C4′ 1Σu1(0) - X 1Σ g+(0) emission band. Estimates of the total electron excitation rates for the nominal b′ 1Σu +(1) and c4′ 1Σu +(0) levels are determined from the spectrum by extrapolating the model through regions containing unmeasured and/or resonantly absorbed bands.
AB - Terrestrial thermospheric dayglow emission from the coupled and overlapping c4′ 1Σu+-(0) and b′ 1Σu+(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′ 1Σu1(0) ∼ b′ 1Σu+(1) - X1 Σg+ (vi = 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 N 2 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′ 1Σu1(0) ∼ b′ 1Σu+(1) - X 1Σ g+(0) band is ∼1% of that inferred from the emission rates to X 1Σg+(vi > 2) levels. A qualitative explanation is given for the drastically reduced intensity and band shape distortion observed in the C4′ 1Σu1(0) - X 1Σ g+(0) emission band. Estimates of the total electron excitation rates for the nominal b′ 1Σu +(1) and c4′ 1Σu +(0) levels are determined from the spectrum by extrapolating the model through regions containing unmeasured and/or resonantly absorbed bands.
UR - http://www.scopus.com/inward/record.url?scp=67649221800&partnerID=8YFLogxK
U2 - 10.1029/2008JD010403
DO - 10.1029/2008JD010403
M3 - Article
SN - 0148-0227
VL - 114
JO - Journal of Geophysical Research
JF - Journal of Geophysical Research
IS - 7
M1 - D07304
ER -