Fig. A.1.

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Evolution of the averaged abundances of the fictitious particles during the convective s-process in a 3M⊙, [Fe/H]=-2.5 star using the large network (Large; solid line), the fictitious network without modifications (Fictitious; dashed line), and the fictitious network with approximated reaction rates (Fictitious + Approx; dotted line). The abundances are averaged over the maximum extent of the convective shell (0.810 ≤ Mr/M⊙ ≤ 0.817528). The mean abundance Yvhs is multiplied by 10−0.2 to distinguish it from Yhse. The thermal pulse starts at model 60609 and ends at model 61002, corresponding to a duration of 39 years.
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