New measurement of neutron capture resonances in 209Bi

被引:46
|
作者
Domingo-Pardo, C. [1 ]
Abbondanno, U.
Aerts, G.
Alvarez-Pol, H.
Alvarez-Velarde, F.
Andriamonje, S.
Andrzejewski, J.
Assimakopoulos, P.
Audouin, L.
Badurek, G.
Baumann, P.
Becvar, F.
Berthoumieux, E.
Calvino, F.
Cano-Ott, D.
Capote, R.
de Albornoz, A. Carrillo
Cennini, P.
Chepel, V.
Chiaveri, E.
Colonna, N.
Cortes, G.
Couture, A.
Cox, J.
Dahlfors, M.
David, S.
Dillman, I.
Dolfini, R.
Dridi, W.
Duran, I.
Eleftheriadis, C.
Embid-Segura, M.
Ferrant, L.
Ferrari, A.
Ferreira-Marques, R.
Fitzpatrick, L.
Frais-Koelbl, H.
Fujii, K.
Furman, W.
Gallino, R.
Goncalves, I.
Gonzalez-Romero, E.
Goverdovski, A.
Gramegna, F.
Griesmayer, E.
Guerrero, C.
Gunsing, F.
Haas, B.
Haight, R.
Heil, M.
机构
[1] Univ Valencia, CSIC, Inst Fis Corpuscular, Valencia, Spain
[2] Ist Nazl Fis Nucl, Trieste, Italy
[3] CEA Saclay, DSM, Gif Sur Yvette, France
[4] Univ Santiago de Compostela, Santiago De Compostela, Spain
[5] Ctr Invest Energet Medioambientales & Technol, Madrid, Spain
[6] Univ Lodz, PL-90131 Lodz, Poland
[7] Univ Ioannina, GR-45110 Ioannina, Greece
[8] Vienna Univ Technol, Atominst Osterr Univ, Vienna, Austria
[9] CNRS, IN2P3, IReS, Strasbourg, France
[10] Charles Univ Prague, Prague, Czech Republic
[11] Univ Politecn Cataluna, Barcelona, Spain
[12] IAEA, NAPC Nucl Data Sect, Vienna, Austria
[13] Univ Seville, Seville, Spain
[14] ITN, Lisbon, Portugal
[15] CERN, Geneva, Switzerland
[16] Univ Coimbra, LIP Coimbra, Coimbra, Portugal
[17] Univ Coimbra, Dept Fis, P-3000 Coimbra, Portugal
[18] Ist Nazl Fis Nucl, I-70126 Bari, Italy
[19] Univ Notre Dame, Notre Dame, IN 46556 USA
[20] CNRS, IPN, IN2P3, Orsay, France
[21] Univ Pavia, I-27100 Pavia, Italy
[22] Aristotle Univ Thessaloniki, GR-54006 Thessaloniki, Greece
[23] Joint Inst Nucl Res, Frank Lab Neutron Phys, Dubna, Russia
[24] Univ Turin, Dipartimento Fis, Turin, Italy
[25] Sezione Ist Nazl Fis Nucl, Turin, Italy
[26] Inst Phys & Power Engn, Obninsk, Russia
[27] Ist Nazl Fis Nucl, Lab Nazl Legnaro, Legnaro, Italy
[28] CNRS, IN2P3, CENBG, Bordeaux, France
[29] Los Alamos Natl Lab, Los Alamos, NM USA
[30] Tokyo Inst Technol, Tokyo 152, Japan
[31] Oak Ridge Natl Lab, Div Phys, Oak Ridge, TN 37831 USA
[32] NCSR, Athens, Greece
[33] Japan Atom Energy Res Inst, Tokai, Ibaraki 31911, Japan
[34] Natl Tech Univ Athens, Athens, Greece
[35] Univ Vienna, Inst Isotopenforsch & Kernphys, Vienna, Austria
[36] Pole Univ Leonard De Vinci, Paris, France
[37] CEC, JRC, IRMM, Geel, Belgium
[38] Univ Basel, Dept Phys & Astron, Basel, Switzerland
[39] ENEA, Bologna, Italy
[40] Univ Bologna, Dipartimento Fis, Bologna, Italy
[41] Sezione Ist Nazl Fis Nucl, Bologna, Italy
来源
PHYSICAL REVIEW C | 2006年 / 74卷 / 02期
关键词
D O I
10.1103/PhysRevC.74.025807
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The neutron capture cross section of Bi-209 has been measured at the CERN n_TOF facility by employing the pulse-height-weighting technique. Improvements over previous measurements are mainly because of an optimized detection system, which led to a practically negligible neutron sensitivity. Additional experimental sources of systematic error, such as the electronic threshold in the detectors, summing of gamma-rays, internal electron conversion, and the isomeric state in bismuth, have been taken into account. gamma-Ray absorption effects inside the sample have been corrected by employing a nonpolynomial weighting function. Because Bi-209 is the last stable isotope in the reaction path of the stellar s-process, the Maxwellian averaged capture cross section is important for the recycling of the reaction flow by alpha decays. In the relevant stellar range of thermal energies between kT=5 and 8 keV our new capture rate is about 16% higher than the presently accepted value used for nucleosynthesis calculations. At this low temperature an important part of the heavy Pb-Bi isotopes are supposed to be synthesized by the s-process in the He shells of low mass, thermally pulsing asymptotic giant branch stars. With the improved set of cross sections we obtain an s-process fraction of 19 +/- 3% of the solar bismuth abundance, resulting in an r-process residual of 81 +/- 3%. The present (n,gamma) cross-section measurement is also of relevance for the design of accelerator driven systems based on a liquid metal Pb/Bi spallation target.
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页数:10
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