Intensity ratio of the 6300 angstrom units and 5577 angstrom units OI emissions in quiet aurora.
Quiet aurora atomic O red and green lines intensity ratio measured from rocket
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Quiet aurora atomic O red and green lines intensity ratio measured from rocket
Helium in atmosphere, aurora and solar wind, discussing geophysical problems, interplanetary neutral H, etc
Mantle aurora caused by auroral electron drift and precipitation
Altitude profiles and absolute intensities of far UV emission features in aurora measured by filterwheel photometer in Aerobee rocket, determining molecular oxygen densities
Visual aurora properties attributed to magnetic storm following solar flare, using multiple channel photometer measurements
Excitation and radiative transport of 1304 A triplet of atomic oxygen for dayglow and aurora
Lower E region recombination coefficients from electron density and flux measurements in glow aurora by Nike-Apache rocket
Secondary electron emission measurement in aurora using Aerobee rocket vehicle
Airborne multifilter scanning photometer data on sunlit auroras
Failure of rocket flown electron accelerator to create artificial aurora
Analysis of N2A 3 Sigma u positive molecule deactivation in auroras using atmospheric model based on mass spectrometer measurements
Nitrogen Vegard-Kaplan and second positive band systems emission, using rocket-borne spectrometer in UV aurora
Differential secondary electron flux measurement in aurora with Aerobee rocket spectrometer
Spatial distribution of aurorae in O and molecular nitrogen ion emissions
Electrojet currents association with visible aurorae, using sounding rockets with rubidium vapor magnetometers
Newly measured electron impact cross sections for excitation of the a 1 Delta g and b 1 Sigma g+ electronic states of O2 were employed to predict the absolute volume emission rates from these states under auroral conditions. A secondary electron electron flux typical of an IBC II nighttime aurora was used and the most important quenching processes were included in the calculations. The new excitation cross sections for the a 1 Delta g and b 1 Sigma g+ states are more than an order of magnitude larger than previous estimates, and lead to correspondingly greater intensities in the atmospheric and IR-atmospheric band systems. The calculated intensity ratios of the volume emission rates of 7621 A and 1.27 microns to that for 3914 A are smaller than obtained from aircraft observations and recent rocket experiments.
Two static mathematical models of the open or Dungey model of the magnetosphere are constructed. The process of construction is similar to that for early closed magnetosphere models, such as the Taylor-Hones model. The first model in fact is simply an addition of an interplanetary field in arbitrary direction to a Taylor-Hones image dipole model. In order to preserve the shape of the magnetosphere at high latitudes, and to partially exclude the exterior field, another model is constructed with the magnetopause approximated by a diamagnetic sphere. We find that there are some interplanetary field lines connected to the earth for all orientations of the interplanetary field other than strictly northward, and that the maximum number of connected field lines occurs with a due southward field. For an average spiral hose angle of the interplanetary field, the dayside neutral point occurs on the magnetopause at about 10 o'clock local time. Dayside auroras, convection patterns, and other phenomena may exhibit symmetry about this local time. For a positive (negative) interplanetary field sector, energetic, anisotropic particle fluxes should have direct access to the northern (southern) polar caps, as is supported by many recent observations.