Status and future directions for direct cross-section measurements of the 13C(a,n)16O reaction for astrophysics

IF 4.3 3区 材料科学 Q1 ENGINEERING, ELECTRICAL & ELECTRONIC
L Csedreki, Gy Gyürky, D Rapagnani, G F Ciani, M Aliotta, C Ananna, L Barbieri, F Barile, D Bemmerer, A Best, A Boeltzig, C Broggini, C G Bruno, A Caciolli, F Casaburo, F Cavanna, P Colombetti, A Compagnucci, P Corvisiero, T Davinson, R Depalo, A Di Leva, Z Elekes, F Ferraro, A Formicola, Zs Fülöp, G Gervino, A Guglielmetti, C Gustavino, G Imbriani, M Junker, M Lugaro, P Marigo, J Marsh, E Masha, R Menegazzo, V Paticchio, R Perrino, D Piatti, P Prati, D Robb, L Schiavulli, R S Sidhu, J Skowronski, O Straniero, T Szücs, S Zavatarelli
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引用次数: 0

Abstract

The 13C(α,n)16O reaction is the main neutron source of the s-process taking place in thermally pulsing AGB stars and it is one of the main candidate sources of neutrons for the i-process in the astrophysical sites proposed so far. Therefore, its rate is crucial to understand the production of the nuclei heavier than iron in the Universe. For the first time, the LUNA collaboration was able to measure the 13C(α,n)16O cross section at E c.m. = 0.23−0.3 MeV drastically reducing the uncertainty of the S(E)-factor in the astrophysically relevant energy range. In this paper, we provide details and critical thoughts about the LUNA measurement and compare them with the current understanding of the 13C(α,n)16O reaction in view of future prospect for higher energy measurements. The two very recent results (from the University of Notre Dame and the JUNA collaboration) published after the LUNA data represent an important step forward. There is, however, still room for a lot of improvement in the experimental study of the 13C(α,n)16O reaction, as emphasized in the present manuscript. We conclude that to provide significantly better constraints on the low-energy extrapolation, experimental data need to be provided over a wide energy range, which overlaps with the energy range of current measurements. Furthermore, future experiments need to focus on the proper target characterisation, the determination of neutron detection efficiency having more nuclear physics input, such as angular distribution of the 13C(α,n)16O reaction below E α < 0.8 MeV and study of nuclear properties of monoenergetic neutron sources and/or via the study of sharp resonances of 13C(α,n)16O. Moreover, comprehensive, multichannel R-matrix analysis with a proper estimate of uncertainty budget of experimental data are still required.
用于天体物理学的 13C(a,n)16O 反应直接截面测量的现状和未来方向
13C(α,n)16O反应是发生在热脉动AGB恒星中的s过程的主要中子源,也是迄今为止提出的天体物理场所中i过程的主要候选中子源之一。因此,它的速率对于了解宇宙中比铁更重的原子核的产生至关重要。LUNA 合作小组首次测量了 Ec.m. = 0.23-0.3 MeV 的 13C(α,n)16O 截面,大大降低了天体物理学相关能量范围内 S(E) 因子的不确定性。在本文中,我们提供了有关 LUNA 测量的细节和批判性思考,并将其与目前对 13C(α,n)16O反应的理解进行了比较,以展望未来更高能量测量的前景。在 LUNA 数据之后发表的两个最新结果(来自圣母大学和 JUNA 合作组织)代表了向前迈出的重要一步。然而,正如本手稿所强调的,13C(α,n)16O 反应的实验研究仍有很大的改进空间。我们的结论是,要想对低能外推法提供明显更好的约束,需要提供宽能量范围的实验数据,这与当前测量的能量范围是重叠的。此外,未来的实验还需要关注正确的目标特征描述,确定中子探测效率和更多的核物理输入,如 Eα < 0.8 MeV 以下 13C(α,n)16O 反应的角度分布,以及研究单能量中子源的核特性和/或通过研究 13C(α,n)16O 的尖锐共振。此外,还需要进行全面的多通道 R 矩阵分析,并对实验数据的不确定性预算进行适当估算。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
7.20
自引率
4.30%
发文量
567
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