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Fig. 3

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Electron (open circles) and hydrogen (filled circles) collision rates of representative transitions in Fe i (left column) and Fe ii (right column) as a function of the transition energy in the model 5780/4.44/0 at a depth point of log τ5000 = −0.5, where T = 5583 K, nH = 0.922 × 1017, and ne = 0.137 × 1014 (top row), and in the model 4600/1.60/−2.50 at a depth point of log τ5000 = −0.5, where T = 4174 K, nH = 0.212 × 1017, and ne = 0.286 × 1011 (bottom row). We assumed SH = 0.1 throughout.

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