Fig. 15.
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Same as Fig. 3, but now comparing the GK simulation against the same run but including a polar jet (jet), and considering only the material ejected within θ ≲ 15 degrees. The abundances are normalized such that the cumulative abundance of the second r-process peak (111 ≤ A ≤ 145) is unity. The histogram shows the cumulative mass fractions for the simulation with the polar jet.
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