High-resolution Cross Section Measurements for Neutron Interactions on ^89 Y with Incident Neutron Energies Up to 95 Kev

G. Tagliente,P. M. Milazzo,C. Paradela,S. Kopecky,D. Vescovi,G. Alaerts,L. A. Damone,J. Heyse,M. Krtička,P. Schillebeeckx,A. Mengoni,R. Wynants,S. Valenta,O. Aberle,V. Alcayne,S. Amaducci,J. Andrzejewski,L. Audouin,V. Babiano-Suarez,M. Bacak,M. Barbagallo,V. Bécares,F. Bečvář,G. Bellia,E. Berthoumieux,J. Billowes,D. Bosnar,A. S. Brown,M. Busso,M. Caamaño,L. Caballero,M. Calviani,F. Calviño,D. Cano-Ott,A. Casanovas,F. Cerutti,Y. H. Chen,E. Chiaveri,N. Colonna,G. P. Cortés,M. A. Cortés-Giraldo,L. Cosentino,S. Cristallo,M. Diakaki,M. Dietz,C. Domingo-Pardo,R. Dressler,E. Dupont,I. Durán,Z. Eleme,B. Fernández-Domíngez,A. Ferrari,I. Ferro-Gonçalves,P. Finocchiaro,V. Furman,R. Garg,A. Gawlik,S. Gilardoni,T. Glodariu,K. Göbel,E. González-Romero,C. Guerrero,F. Gunsing,S. Heinitz,D. G. Jenkins,E. Jericha,Y. Kadi,F. Käppeler,A. Kimura,N. Kivel,M. Kokkoris,Y. Kopatch,D. Kurtulgil,I. Ladarescu,A. C. Larsen,C. Lederer-Woods,J. Lerendegui-Marco,S. Lo Meo,S. J. Lonsdale,M. Lugaro,D. Macina,A. Manna,T. Martínez,A. Masi,C. Massimi,P. F. Mastinu,M. Mastromarco,F. Matteucci,E. Maugeri,A. Mazzone,E. Mendoza,V. Michalopoulou,F. Mingrone,A. Musumarra,A. Negret,R. Nolte,F. Ogállar,A. Oprea,N. Patronis,A. Pavlik,J. Perkowski,L. Piersanti,I. Porras,J. Praena,J. M. Quesada,D. Radeck,D. Ramos Doval,R. Reifarth,D. Rochman,C. Rubbia,M. Sabaté-Gilarte,A. Saxena,D. Schumann,A. G. Smith,M. Spelta,N. Sosnin,A. Stamatopoulos,J. L. Tain,Z. Talip,A. E. Tarifeño-Saldivia,L. Tassan-Got,P. Torres-Sánchez,A. Tsinganis,J. Ulrich,S. Urlass,G. Vannini,V. Variale,P. Vaz,A. Ventura,V. Vlachoudis,R. Vlastou,A. Wallner,P. J. Woods,T. J. Wright,P. Žugec

The European Physical Journal A(2024)

引用 0|浏览46
暂无评分
摘要
The cross section of the ^89 Y(n, γ ) reaction has important implications in nuclear astrophysics and for advanced nuclear technology. Given its neutron magic number N = 50 and a consequent small neutron capture cross section, ^89 Y represents one of the key nuclides for the stellar s-process. It acts as a bottleneck in the neutron capture chain between the Fe seed and the heavier elements. Moreover, it is located at the overlapping region, where both the weak and main s-process components take place. ^89 Y, the only stable yttrium isotope, is also used in innovative nuclear reactors. Neutron capture and transmission measurements were performed at the time-of-flight facilities n_TOF at CERN and GELINA at JRC-Geel. Resonance parameters of individual resonances were extracted from a resonance analysis of the experimental transmission and capture yields, up to a neutron incident energy of 95 keV. Even though a comparison with results reported in the literature shows differences in resonance parameters, the present data are consistent with the Maxwellian averaged cross section suggested by the astrophysical database KADoNiS.
更多
查看译文
关键词
Astrophysical Reaction Rates
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要