Approaching the precursor nuclei of the third r-process peak with RIBs
The rapid neutron nucleosynthesis process involves an enormous amount of very exotic neutron-rich nuclei, which represent a theoretical and experimental challenge. Two of the main decay properties that affect the final abundance distribution the most are half-lives and neutron branching ratios. Usin...
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Published in | Journal of physics. Conference series Vol. 665; no. 1; pp. 12045 - 12052 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Abstract | The rapid neutron nucleosynthesis process involves an enormous amount of very exotic neutron-rich nuclei, which represent a theoretical and experimental challenge. Two of the main decay properties that affect the final abundance distribution the most are half-lives and neutron branching ratios. Using fragmentation of a primary 238U beam at GSI we were able to measure such properties for several neutron-rich nuclei from 208Hg to 218Pb. This contribution provides a short update on the status of the data analysis of this experiment, together with a compilation of the latest results published in this mass region, both experimental and theoretical. The impact of the uncertainties connected with the beta-decay rates and with beta-delayed neutron emission is illustrated on the basis of r-process network calculations. In order to obtain a reasonable reproduction of the third r-process peak, it is expected that both half-lives and neutron branching ratios are substantially smaller, than those based on FRDM+QRPA, commonly used in r-process model calculations. Further measurements around N ∼ 126 are required for a reliable modelling of the underlying nuclear structure, and for performing more realistic r-process abundance calculations. |
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AbstractList | The rapid neutron nucleosynthesis process involves an enormous amount of very exotic neutron-rich nuclei, which represent a theoretical and experimental challenge. Two of the main decay properties that affect the final abundance distribution the most are half-lives and neutron branching ratios. Using fragmentation of a primary 238U beam at GSI we were able to measure such properties for several neutron-rich nuclei from 208Hg to 218Pb. This contribution provides a short update on the status of the data analysis of this experiment, together with a compilation of the latest results published in this mass region, both experimental and theoretical. The impact of the uncertainties connected with the beta-decay rates and with beta-delayed neutron emission is illustrated on the basis of r-process network calculations. In order to obtain a reasonable reproduction of the third r-process peak, it is expected that both half-lives and neutron branching ratios are substantially smaller, than those based on FRDM+QRPA, commonly used in r-process model calculations. Further measurements around N ∼ 126 are required for a reliable modelling of the underlying nuclear structure, and for performing more realistic r-process abundance calculations. |
Author | Wood, R Scheidenberger, Ch Montes, F Mukha, I Farinon, F Prochazka, A Napoli, D R Maier, L Martínez, T Guerrero, C Galaviz, D Ayyad, Y Litvinov, Y Winfield, J S Davinson, T Gelletly, W Martínez-Pinedo, G Gómez-Hornillos, M B Paradela, C Faestermann, T Kojouharov, I Woods, P Evdokimov, A Steiger, K Cano-Ott, D Bowry, M Podolyák, Z Schaffner, H Pietri, S Weick, H Domingo-Pardo, C Marta, M Nociforo, Ch Yeremin, A Geissel, H Agramunt, J Taín, J L Takechi, M Heil, M Rice, S Meyer, B S Knöbel, R Ameil, F Kurz, N Kurcewicz, J García-Rios, A Cortés, G Calviño, F Gernhäuser, R Smith, K Caballero-Folch, R Hinke, C Rubio, B Sun, B Testov, D Arcones, A Benlliure, J Riego, A Wilson, E Algora, A Dillmann, I Marganiec, J Estrade, A Sokol, E |
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SubjectTerms | Beta decay Data analysis Decay rate Half-life Neutron emission Neutrons Nuclear fusion Nuclear structure Nuclei Physics |
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Title | Approaching the precursor nuclei of the third r-process peak with RIBs |
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