The neutron capture cross section of Pb-206 has been measured at the CERN n_TOF spectrometer using a setup of two C6D6 detectors. In the energy interval from 1 eV to 600 keV the cross section is dominated by resonances, which were analyzed via the R-matrix analysis code SAMMY. In the relevant energy ranges for stellar nucleosynthesis, i. e., at thermal energies of kT = 8 keV and kT = 23 keV, the present Maxwellian average cross section differs by 20% and 9% from the recommended values of Bao et al respectively. From the new cross section the s-abundance of Pb-206 could be reliably determined as 70( 4)%. This result is of importance in order to test and constrain r-process abundance calculations in the actinide region, because the r-process portion of Pb-206 is dominated by alpha-back decays of short-lived transbismuth isotopes.

The measurement of the Pb-206(n,gamma) cross section and stellar implications

BISTERZO, SARA;FERRARI, Attilio;GALLINO, Roberto;
2008-01-01

Abstract

The neutron capture cross section of Pb-206 has been measured at the CERN n_TOF spectrometer using a setup of two C6D6 detectors. In the energy interval from 1 eV to 600 keV the cross section is dominated by resonances, which were analyzed via the R-matrix analysis code SAMMY. In the relevant energy ranges for stellar nucleosynthesis, i. e., at thermal energies of kT = 8 keV and kT = 23 keV, the present Maxwellian average cross section differs by 20% and 9% from the recommended values of Bao et al respectively. From the new cross section the s-abundance of Pb-206 could be reliably determined as 70( 4)%. This result is of importance in order to test and constrain r-process abundance calculations in the actinide region, because the r-process portion of Pb-206 is dominated by alpha-back decays of short-lived transbismuth isotopes.
2008
NUCLEAR PHYSICS IN ASTROPHYSICS III (TECHNISCHE UNIVERSITÄT DRESDEN, GERMANY, 26--31 MARCH 2007)
DRESDEN
26--31 MARCH 2007
35
014020
-
C. Domingo-Pardo;U. Abbondanno;G. Aerts;H. Alvarez;F. Alvarez-Velarde;S. Andriamonje;J. Andrzejewski;P. Assimakopoulos;L. Audouin;G. Badurek;P. Baumann;F. Becvar;E. Berthoumieux;S. Bisterzo;F. Calvino;M. Calviani;D. Cano-Ott;R. Capote;C. Carrapico;P. Cennini;V. Chepel;N. Colonna;G. Cortes;A. Couture;J. Cox;M. Dahlfors;S. David;I. Dillmann;W. Dridi;I. Duran;C. Eleftheriadis;M. Embid-Segura;L. Ferrant;A. Ferrari;R. Ferreira-Marques;K. Fujii;W. Furman;R. Gallino;I. Goncalves;E. Gonzalez-Romero;F. Gramegna;C. Guerrero;F. Gunsing;B. Haas;R. Haight;M. Heil;A. Herrera-Martinez;M. Igashira;E. Jericha;Y. Kadi;F. Kappeler;D. Karadimos;D. Karamanis;M. Kerveno;P. Koehler;E. Kossionides;M. Krticka;C. Lamboudis;H. Leeb;A. Lindote;I. Lopes;M. Lozano;S. Lukic;J. Marganiec;S. Marrone;C. Massimi;P. Mastinu;A. Mengoni;P. M. Milazzo;M. Mosconi;F. Neves;H. Oberhummer;S. O'Brien;J. Pancin;C. Papachristodoulou;C. Papadopoulos;C. Paradela;N. Patronis;A. Pavlik;P. Pavlopoulos;L. Perrot;M. T. Pigni;R. Plag;A. Plompen;A. Plukis;A. Poch;C. Pretel;J. Quesada;T. Rauscher;R. Reifarth;C. Rubbia;G. Rudolf;P. Rullhusen;J. Salgado;C. Santos;L. Sarchiapone;I. Savvidis;C. Stephan;G. Tagliente;J. L. Tain;L. Tassan-Got;L. Tavora;R. Terlizzi;G. Vannini;P. Vaz;A. Ventura;D. Villamarin;M. C. Vincente;V. Vlachoudis;R. Vlastou;F. Voss;S. Walter;M. Wiescher;K. Wisshak
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/65658
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