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note
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The difference between the rate coefficients for direct (dashed line) and total (dotted line) processes in Fig. 9c may seem large when compared to the resonance structure in Fig. 9b above. This is due to the different scales between the two figures, and also to the logarithmic scales which make the resonances look almost symmetric in Fig. 9b while actually their positive parts are much larger than the dip ones and lead to an appreciable increase of the rate after Maxwell averaging.
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