The neutron capture cross section of (206)Pb has been measured at the CERN n_TOF spectrometer using a setup of two C(6)D(6) 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 (206)Pb 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 (206)Pb is dominated by alpha-back decays of short-lived transbismuth isotopes.

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

MASSIMI, CRISTIAN;VANNINI, GIANNI;
2008

Abstract

The neutron capture cross section of (206)Pb has been measured at the CERN n_TOF spectrometer using a setup of two C(6)D(6) 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 (206)Pb 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 (206)Pb is dominated by alpha-back decays of short-lived transbismuth isotopes.
2008
C Domingo-Pardo;U Abbondanno;G Aerts;H Álvarez;F Alvarez-Velarde;S Andriamonje;J Andrzejewski;P Assimakopoulos;L Audouin;G Badurek;P Baumann;F Bečvář;E Berthoumieux;S Bisterzo;F Calviño;M Calviani;D Cano-Ott;R Capote;C Carrapiço;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 Käppeler;D Karadimos;D Karamanis;M Kerveno;P Koehler;E Kossionides;M Krtička;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/11585/140205
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