The recent level population calculations for Ne v by Aggarwal are used to determine the theoretical emission line ratios RI = l(2s2p 3 ID~ -2s22p 2 lDe)/I(2s2p3 3D~ -2sZ2p ~ 3p~) and Rz = i(2s2p3 1DO \_ 2sZ2pZ lDe)/l(2s2p3 3DO \_ 2s~2p2 3p~). A comparison of these with observational data for a solar
Theoretical emission line ratios for SiXIIIcompared to solar observations
โ Scribed by S. M. McCann; F. P. Keenan
- Publisher
- Springer
- Year
- 1987
- Tongue
- English
- Weight
- 282 KB
- Volume
- 112
- Category
- Article
- ISSN
- 0038-0938
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โฆ Synopsis
The electron collision excitation rates recently calculated for transitions in Si xIII by Keenan et al. (1987) are used to derive the electron temperature sensitive ratio G( = (f + i)/r) and the density sensitive ratio R(=f/i), where i,f, and r are the intercombination (ls 2 1S -ls2p 3P1, 2) forbidden (ls 2 1S -ls2s 3S), and resonance (ls 2 ~S -ls2p 1p), transitions respectively. Also estimated are the values of R in the low-density limit (Ro) as a function of electron temperature. The theoretical G ratio at the temperature of maximum emissivity for SixIIL G(Tm) = 0.70, is in much better agreement with the observed G for the 1985, May 5 flare determined by McKenzie et al. (G = 0.60 + 0.07) than is the earlier calculation of Pradhan, who derived G(Tm) = 0.85. The error in the observed Ro ratio is so large that both our result and Pradhan's fall within the acceptable limits of uncertainty and hence one cannot estimate which of the two is the more accurate.
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