重新测量霍伊尔态的γ$衰变分支率

W. Paulsen, K. C. W. Li, S. Siem, V. W. Ingeberg, A. C. Larsen, T. K. Eriksen, H. C. Berg, M. M. Bjørøen, B. J. Coombes, J. T. H. Dowie, F. W. Furmyr, F. L. B. Garrote, D. Gjestvang, A. Görgen, T. Kibédi, M. Markova, V. Modamio, E. Sahin, A. E Stuchbery, G. M. Tveten, V. M. Valsdòttir
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引用次数: 0

摘要

霍伊尔态的辐射支化比对于估算恒星环境中中等温度下的三($\alpha$)反应速率至关重要。Kib\'edi 等人最近的一项研究[Phys. Rev. Lett. 125, 182701 (2020)]挑战了我们对这一具有重大物理意义的分支比及其约束条件的理解。这项工作的目的是对霍伊尔态的γ衰变分支进行新的测量,以推导出霍伊尔态的辐射分支比。在这项工作的主要实验中,霍伊尔态是由奥斯陆回旋加速器实验室在10.8MeV下的$^{12}\textrm{C}(p,p')$反应填充的。伽马射线衰变率是通过三重共振事件推导出来的,每一个共振事件都包括与霍伊尔态相对应的质子抛射物以及随后的伽马射线级联。在这项工作的主要实验中,确定了霍伊尔态的$\gamma$-decay支化比为$\Gamma_{\gamma}/\Gamma=4.0(4)\times10^{-4}$,得出了相应的辐射支化比为$\Gamma_{textrm{rad}}/\Gamma=4.0(4)\times10^{-4}$。1(4) \times 10^{-4}$,这与最近的几项研究以及之前采用的 ENSDF 平均值$\Gamma_{textrm{rad}}/\Gamma=4.16(11)\times 10^{-4}$相一致。Kib\'edi 等人所做分析的某些方面在这项工作中得到了验证,但无法确定这项工作的结果与 Kib\'edi 等人的结果之间存在差异的原因。对霍伊尔态辐射宽度的进一步独立和创新研究将证实是否应在未来的评估中排除Kib\'edi 等人的差异结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Remeasuring the $γ$-decay branching ratio of the Hoyle state
The radiative branching ratio of the Hoyle state is crucial to estimate the triple-$\alpha$ reaction rate in stellar environments at medium temperatures. Knowledge of the $\gamma$-decay channel is critical as this is the dominant radiative decay channel for the Hoyle state. A recent study by Kib\'edi et al. [Phys. Rev. Lett. 125, 182701 (2020)] has challenged our understanding of this astrophysically significant branching ratio and its constraints. The objective of this work was to perform a new measurement of the $\gamma$-decay branching ratio of the Hoyle state to deduce the radiative branching ratio of the Hoyle state. An additional objective was to independently verify aspects of the aforementioned measurement conducted by Kib\'edi et al. For the main experiment of this work, the Hoyle state was populated by the $^{12}\textrm{C}(p,p')$ reaction at 10.8 MeV at the Oslo Cyclotron Laboratory. The $\gamma$-decay branching ratio was deduced through triple-coincidence events, each consisting of a proton ejectile corresponding to the Hoyle state, and the subsequent $\gamma$-ray cascade. In the main experiment of this work, a $\gamma$-decay branching ratio of the Hoyle state of $\Gamma_{\gamma}/\Gamma=4.0(4)\times 10^{-4}$ was determined, yielding a corresponding radiative branching ratio of $\Gamma_{\textrm{rad}}/\Gamma=4.1(4) \times 10^{-4}$, which is in agreement with several recent studies, as well as the previously adopted ENSDF average of $\Gamma_{\textrm{rad}}/\Gamma=4.16(11)\times 10^{-4}$. Aspects of the analysis performed by Kib\'edi et al. were verified in this work and the source of discrepancy between the results of this work and that of Kib\'edi et al. could not be determined. Further independent and innovative studies for the radiative width of the Hoyle state will substantiate whether the discrepant result by Kib\'edi et al. should be excluded from future evaluations.
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