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Approaching the precursor nuclei of the third r-process peak with RIBs

Authors :
Domingo-Pardo, C.
Caballero-Folch, R.
Agramunt, J.
Algora, A.
Arcones, A.
Ameil, F.
Ayyad, Y.
Benlliure, J.
Bowry, M.
Calviño, F.
Cano-Ott, D.
Cortés, G.
Davinson, T.
Dillmann, I.
Estrade, A.
Evdokimov, A.
Faestermann, T.
Farinon, F.
Galaviz, D.
García-Rios, A.
Geissel, H.
Gelletly, W.
Gernhäuser, R.
Gómez-Hornillos, M. B.
Guerrero, C.
Heil, M.
Hinke, C.
Knöbel, R.
Kojouharov, I.
Kurcewicz, J.
Kurz, N.
Litvinov, Y.
Maier, L.
Marganiec, J.
Marta, M.
Martínez, T.
Martínez-Pinedo, G.
Meyer, B. S.
Montes, F.
Mukha, I.
Napoli, D. R.
Nociforo, Ch.
Paradela, C.
Pietri, S.
Podolyák, Z.
Prochazka, A.
Rice, S.
Riego, A.
Rubio, B.
Schaffner, H.
Scheidenberger, Ch.
Smith, K.
Sokol, E.
Steiger, K.
Sun, B.
Taín, J. L.
Takechi, M.
Testov, D.
Weick, H.
Wilson, E.
Winfield, J. S.
Wood, R.
Woods, P.
Yeremin, A.
Publication Year :
2013

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 $^{238}$U beam at GSI we were able to measure such properties for several neutron-rich nuclei from $^{208}$Hg to $^{218}$Pb. 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 $N\sim126$ are required for a reliable modelling of the underlying nuclear structure, and for performing more realistic $r$-process abundance calculations.<br />Comment: Nuclear Physics in Astrophysics VI, Lisbon 2013, Conference Proceedings

Subjects

Subjects :
Nuclear Experiment

Details

Database :
arXiv
Publication Type :
Report
Accession number :
edsarx.1309.3047
Document Type :
Working Paper