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Fig. 8

image

Abundances inferred at the different μ-pointings using the ⟨3D⟩ model solar atmosphere. The same abundance should be inferred from each μ-pointing (i.e. a flat line is expected). Left panel: effect of altering all inelastic O+e or O+H excitation rate coefficients. Right panel: effect of altering the inelastic O+e and O+H excitation rate coefficients (simultaneously) for the specified transition.

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