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Fig. A.1

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Formation of the strongest C I lines in the visible from the multiplet 270; λλ 9 061, 9 062, 9 078, 9 089, 9 095, 9 112 Å. The level 2s2 2p3s is strongly populated by the UV resonance transition, which al- lows the absorption lines to the level 2s22p3p. However, the upper level from this transition is also populated from the level 2s2 2p3d pumped by UV radiation. This overpopulation of 2s22p3p creates the emission wings of these strongest lines.

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