Quantitative spectroscopy of the aurora. IV. The spectrum of medium intensity aurora between 8800 Å and 11 400 Å

1976 ◽  
Vol 54 (21) ◽  
pp. 2128-2133 ◽  
Author(s):  
A. Vallance Jones ◽  
R. L. Gattinger

An averaged spectrum of medium intensity aurora (I(4278 Å) ≈ 20 kR) at a resolution of 15 Å from 8800 Å to 11 400 Å is presented. The observations were made with a grating spectrometer and S1 photomultiplier detector. Synthetic comparison spectra were prepared to aid in the identification and relative intensity measurements of the observed emission features. Included in the synthesis were the nitrogen first positive, Meinel, and infrared afterglow systems, the oxygen atmospheric system, the hydroxyl vibration–rotation system, and a number of atomic emissions. Three unidentified features have been tentatively ascribed to NI multiplets. Comparisons have been made between the observed and theoretically calculated relative populations of the four lowest vibrational levels in the upper electronic states of both the nitrogen first positive and Meinel systems. The relative vibrational populations of N2(B3Π) do not fit the hypothesis of direct electron impact excitation plus cascade through the N2 second positive system. The relative vibrational population rates of the Meinel N2+ system deviate from the Franck–Condon factors for the excitation transition.

1983 ◽  
Vol 61 (2) ◽  
pp. 244-250 ◽  
Author(s):  
D. N. Turnbull ◽  
R. P. Lowe

Relative populations of the vibrational levels ν = 2 to ν = 9 (except ν = 5) of the hydroxyl radical have been determined from observations of the Δν = 2 and 3 sequences of the vibration–rotation bands in the infrared night airglow spectrum using a Fourier transform spectrometer. The observed line intensities were corrected for water vapour absorption using a new technique. The results indicate a population of the upper vibrational levels which is as much as a factor of two lower than that found in other studies. The observed distribution is not consistent with the atomic hydrogen ozone reaction being the sole excitation mechanism in the night airglow unless the quenching and other rates used in our model are in error.


1988 ◽  
Vol 102 ◽  
pp. 129-132
Author(s):  
K.L. Baluja ◽  
K. Butler ◽  
J. Le Bourlot ◽  
C.J. Zeippen

SummaryUsing sophisticated computer programs and elaborate physical models, accurate radiative and collisional atomic data of astrophysical interest have been or are being calculated. The cases treated include radiative transitions between bound states in the 2p4and 2s2p5configurations of many ions in the oxygen isoelectronic sequence, the photoionisation of the ground state of neutral iron, the electron impact excitation of the fine-structure forbidden transitions within the 3p3ground configuration of CℓIII, Ar IV and K V, and the mass-production of radiative data for ions in the oxygen and fluorine isoelectronic sequences, as part of the international Opacity Project.


1988 ◽  
Vol 102 ◽  
pp. 107-110
Author(s):  
A. Burgess ◽  
H.E. Mason ◽  
J.A. Tully

AbstractA new way of critically assessing and compacting data for electron impact excitation of positive ions is proposed. This method allows one (i) to detect possible printing and computational errors in the published tables, (ii) to interpolate and extrapolate the existing data as a function of energy or temperature, and (iii) to simplify considerably the storage and transfer of data without significant loss of information. Theoretical or experimental collision strengths Ω(E) are scaled and then plotted as functions of the colliding electron energy, the entire range of which is conveniently mapped onto the interval (0,1). For a given transition the scaled Ω can be accurately represented - usually to within a fraction of a percent - by a 5 point least squares spline. Further details are given in (2). Similar techniques enable thermally averaged collision strengths upsilon (T) to be obtained at arbitrary temperatures in the interval 0 < T < ∞. Application of the method is possible by means of an interactive program with graphical display (2). To illustrate this practical procedure we use the program to treat Ω for the optically allowed transition 2s → 2p in ArXVI.


2001 ◽  
Vol 11 (PR2) ◽  
pp. Pr2-309-Pr2-312
Author(s):  
K. M. Aggarwal ◽  
F. P. Keenan ◽  
S. J. Rose

1989 ◽  
Vol 50 (C1) ◽  
pp. C1-405-C1-409
Author(s):  
L. D. GARDNER ◽  
J. L. KOHL ◽  
D. W. SAVIN ◽  
A. R. YOUNG

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