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Fig. 7

image

Scheme illustrating the operation of the two branches at 85Kr (ground state) and 86Rb that determine the Rb production by the s-process. Black filled nuclei are stable, while the empty ones are unstable. Arrows show possible nuclear reactions, particularly neutron captures or β-decays. In case of low neutron density (Nn < 109 cm−3), both branches are closed and the s-process follows the chain 84Kr →85Kr →85Rb →86Rb →86Sr. Owing to the large neutron-capture cross section of 85Kr compared to those of the neutron-magic nuclei (N = 50) 88Sr, 89Y, and 90Zr, a low amount of Rb is produced. On the contrary, at higher neutron density, the two branches are open and the s-process sequence deviates toward 86Kr and 87Rb, both of which are neutron magic nuclei, and therefore both present very low neutron-capture cross sections. In the latter case, large overabundances of Kr and Rb are found.

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