在欧洲核子研究中心n_TOF装置上首次测量94Nb(n,γ)截面

J. Balibrea-Correa, V. Babiano-Suárez, J. Lerendegui-Marco, C. Domingo-Pardo, I. Ladarescu, A. Tarifeño-Saldivia, V. Alcayne, D. Cano-Ott, E. Gonz'alez-Romero, T. Mart'inez, E. Mendoza, J. Plaza, A. S'anchez-Caballero, F. Calviño, A. Casanovas, C. Guerrero, S. Heinitz, U. Koster, E. Maugeri, R. Dressler, D. Schumann, I. Monch, S. Cristallo, C. Lederer-Woods, O. Aberle, S. Altieri, S. Amaducci, J. Andrzejewski, M. Bacak, C. Beltrami, S. Bennett, A. Bernardes, E. Berthoumieux, M. Boromiza, D. Bosnar, M. Caamano, M. Calviani, F. Cerutti, G. Cescutti, S. Chasapoglou, E. Chiaveri, P. Colombetti, N. Colonna, P. C. Camprini, G. Cort'es, M. A. Cort'es-Giraldo, L. Cosentino, S. Dellmann, M. D. Castro, S. Maria, M. Diakaki, M. Dietz, E. Dupont, I. Dur'an, Z. Eleme, S. Fargier, B. Fern'andez, B. Fern'andez-Dom'inguez, P. Finocchiaro, S. Fiore, V. Furman, F. Garc'ia-Infantes, A. Gawlik-Ramikega, G. Gervino, S. Gilardoni, F. Gunsing, C. Gustavino, J. Heyse, W. Hillman, D. Jenkins, E. Jericha, A. Junghans, Y. Kadi, K.
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引用次数: 1

摘要

改进恒星模型的关键因素之一是精确了解参与s-、r-和i-过程的不同同位素的中子俘获截面。这些测量可以揭示观测到的和预测的同位素丰度之间存在的差异,并有助于限制这些反应在恒星演化的不同阶段发生的物理条件。在放射性94Nb的特殊情况下,94Nb(n,γ)截面可以在确定AGB恒星中94Mo的s过程产生中发挥作用,目前最先进的恒星模型无法复制。以前没有94Nb(n,γ)的已分辨和未分辨共振区域的实验数据,主要是由于难以产生高质量的样品,也由于在飞行时间实验中常用的传统检测系统的局限性。在这种情况下,在CERN n_TOF进行了94Nb(n,γ)反应的首次测量,从而利用EAR2区域的高亮度,结合小体积c6d6探测器和高质量94Nb样品的新检测系统。后者是基于在ILL-Grenoble高通量反应堆活化的超纯93Nb材料。一个创新的环形配置检测系统,在接近几何形状的捕获样本,使我们能够显著提高信号背景比。该装置补充了两个传统的c6d6探测器和一个高分辨率LaCl3(Ce)探测器,这将用于可靠地解决系统效应和不确定性。在目前数据分析的状态下,94Nb+n首次在热- 10kev中子能量范围内观测到18个共振。
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First measurement of the 94Nb(n,γ) cross section at the CERN n_TOF facility
One of the crucial ingredients for the improvement of stellar models is the accurate knowledge of neutron capture cross-sections for the different isotopes involved in the s-,r- and i- processes. These measurements can shed light on existing discrepancies between observed and predicted isotopic abundances and help to constrain the physical conditions where these reactions take place along different stages of stellar evolution. In the particular case of the radioactive 94Nb, the 94Nb(n,γ) cross-section could play a role in the determination of the s-process production of 94Mo in AGB stars, which presently cannot be reproduced by state-of-the-art stellar models. There are no previous 94Nb(n,γ) experimental data for the resolved and unresolved resonance regions mainly due to the difficulties in producing highquality samples and also due to limitations in conventional detection systems commonly used in time-of-flight experiments. Motivated by this situation, a first measurement of the 94Nb(n,γ) reaction was carried out at CERN n_TOF, thereby exploiting the high luminosity of the EAR2 area in combination with a new detection system of small-volume C6D6-detectors and a high quality 94Nb-sample. The latter was based on hyper-pure 93Nb material activated at the high-flux reactor of ILL-Grenoble. An innovative ring-configuration detection system in close geometry around the capture sample allowed us to significantly enhance the signal-to-background ratio. This set-up was supplemented with two conventional C6D6-detectors and a highresolution LaCl3(Ce)-detector, which will be employed for addressing reliably systematic effects and uncertainties. At the current status of the data analysis, 18 resonance in 94Nb+n have been observed for the first time in the neutron energy range from thermal up to 10 keV.
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