The excitation of the levels 21P, 31D, 51D, 61D and 71D of helium in quiescent prominences and the chromosphere is considered using the observations made during the
Ionized helium in prominences and in the chromosphere
โ Scribed by Tadashi Hirayama
- Publisher
- Springer
- Year
- 1972
- Tongue
- English
- Weight
- 695 KB
- Volume
- 24
- Category
- Article
- ISSN
- 0038-0938
No coin nor oath required. For personal study only.
โฆ Synopsis
It is found that HelI 4686 ,is emitted in ithe same cold region of < 10000 K as hydrogen, metal and neutral helium emission lines. This conclusion is based on the finding that the observed width of 24686 is the same as the calculated width of 24686. The calculated width is derived from the observed widths of hydrogen and metallic lines. The large intensity of Hen 4686 in < 10000 K can be explained by the ionization of Hell due to the UV radiation below 228 that comes from the corona and the transition region.
Loop Prominences: The very broad width (30 to 50 km s -1) of ~.4686 for two post-flare loop prominences shows that the Hell line is emitted in hot regions different from regions of hydrogen and metal emission. From the widths of the Balmer lines and many metallic lines the kinetic temperature for one loop is found to be 16000 K in one part and 7600 K in another part. The electron densities are 1012.~ cm -z and less than 1011-~ cm -~ respectively.
Chromosphere: The intensity of 24686 in the chromosphere can be interpreted in terms of a temperature of < 10000 K with the ionization due to UV radiation. But, since observations of the width of 24686 are not available, a definitive conclusion for the chromosphere cannot be reached.
๐ SIMILAR VOLUMES
Observations of a number of helium triplet (~.210830, 4713, 4471, 3889, 4026) and hydrogea (H),, g, r/, 0) emission line intensities in six quiescent prominences are presented. The regions of prominence and neighboring corona were raster-scanned by the telescope, and all lines were measured concurre
The statistical equilibrium equations for the continuum and first 10 levels of a hydrogen atom show that the radiation of a bright prominence (the brightness of the H~ line has attained 56 m/k of the disc centre spectrum) is completely due to scattering of the Sun radiation. The basic unknowns are s