Solar Gamma-, X-, and EUV Radiation 1975
DOI: 10.1007/978-94-010-1802-9_10
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Interpretation of the X-Ray Spectra of Solar Active Regions

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1975
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Cited by 7 publications
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“…The "kernel" of the integral, K(T.,), which is the convolution of the telescope efficiency and the solar emissivity, is given by a ? sum indexed by element (Z), ionization stage (z), and transition from excited state i to lower state j K(T) = : ic1( X) = : (5) k Zzij where A is the abundance of element Z, a is the fractional population of ionization stage z, and aZZ is the excitation function for transition (i->j) (including all population processes for the upper level i, and branching ratios to the lower level j). These relations only hold for optically thin lines; thus, this derivation is not valid for the 1216 A telescope, which is sensitive to the optically thick Lyman a line6.…”
Section: Solar Emissionmentioning
confidence: 99%
“…The "kernel" of the integral, K(T.,), which is the convolution of the telescope efficiency and the solar emissivity, is given by a ? sum indexed by element (Z), ionization stage (z), and transition from excited state i to lower state j K(T) = : ic1( X) = : (5) k Zzij where A is the abundance of element Z, a is the fractional population of ionization stage z, and aZZ is the excitation function for transition (i->j) (including all population processes for the upper level i, and branching ratios to the lower level j). These relations only hold for optically thin lines; thus, this derivation is not valid for the 1216 A telescope, which is sensitive to the optically thick Lyman a line6.…”
Section: Solar Emissionmentioning
confidence: 99%