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Fig. B.1

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Illustrations of the numerical method employed for implementing N2 (and CO) shielding functions in this work. The plots show the fractional abundances of N2 as functions of radii. It is seen that one can obtain the same converged results (solid lines in black) by assuming N2 is either fully shielded (dashed line in red, left panel) or unshielded (dashed line in blue, right panel) during the first loop. The dotted lines show the intermediate abundances before reaching the final results.

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