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Fig. 7

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Comparison between an intensity calculated as I ≈ ρ2l, where l is the column thickness along the line-of-sight (solid), the base model 171 intensity I171(t) (dotted), and the base model 193 intensity I193(t) (dashed) for a viewing angle of 0° and a pixel size resolution of 0R for ray 2. The differences between the lines illustrates the importance of the Gλ0(T,ne) function.

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