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β-Delayed α Decay of ~(16)N and the ~(12)C(α,γ)~(16)O Cross Section at Astrophysical Energies: a New Experimental Approach

机译:β-延迟α衰减〜(16)n和〜(12)c(α,γ)〜(16)o横截面在天体物理能量:一种新的实验方法

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The ~(12)C(α,γ)~(16)O reaction at energies corresponding to the quiescent helium burning in massive stars is regarded as one of the most important processes in nuclear astrophysics. Although this process has being studied for over four decades, our knowledge of its cross section at the energies of interest for astrophysics is still widely unsatisfactory. Indeed, no experimental data are available around 300 keV and in the energy region of astrophysical interest extrapolations are performed using some theoretical approaches, usually R-matrix calculations. Consequently, the published astrophysical factors range from 1 to 288 keVb for S_(E1)(300) and 7 to 120 keVb for S_(E2)(300), especially because of the unknown contribution coming from subthreshold resonances. To improve the reliability of these extrapolations, data from complementary experiments, such as elastic and quasi- elastic α scattering on ~(12)C, α-transfer reactions to ~(16)O, and ~(16)N decay are usually included in the analysis. Here the β-delayed α decay of ~(16)N is used to infer information on the ~(12)C(α,γ)~(16)O reaction and a new experimental technique is suggested.
机译:对应于在大规模恒星中燃烧的静态氦气相对应的能量的〜(12)C(α,γ)〜(16)o反应被认为是核天体物理学中最重要的过程之一。虽然这一进程已经在四十年中进行了研究,但我们对天体物理学感兴趣的能量的横截面的了解仍然不满意。实际上,在300keV约300keV中没有有实验数据,并且在天体物理学兴趣的能量区域中,使用一些理论方法进行外推,通常是R-矩阵计算。因此,出版的天体物理因子为S_(E1)(300)和S_(E2)(300)的S_(E1)(300)和7至120keVB的范围为7至120keVB,特别是因为来自亚阈值共振的未知贡献。为了提高这些外推的可靠性,通常包括互补实验的数据,例如弹性和准α散射〜(12)c,α-转移反应至〜(16)o,〜(16)n衰减在分析中。这里,〜(16)n的β延迟α衰减用于推断出关于〜(12)C(α,γ)〜(16)O反应的信息,并提出了一种新的实验技术。

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