First direct measurement of the 64.5 keV resonance strength in $^{17}$O(p,$γ$)$^{18}$F reaction

R. M. Gesuè, G. F. Ciani, D. Piatti, A. Boeltzig, D. Rapagnani, M. Aliotta, C. Ananna, L. Barbieri, F. Barile, D. Bemmerer, A. Best, C. Broggini, C. G. Bruno, A. Caciolli, M. Campostrini, F. Casaburo, F. Cavanna, P. Colombetti, A. Compagnucci, P. Corvisiero, L. Csedreki, T. Davinson, G. M. De Gregorio, D. Dell'Aquila, R. Depalo, A. Di Leva, Z. Elekes, F. Ferraro, A. Formicola, Zs. Fülöp, G. Gervino, A. Guglielmetti, C. Gustavino, Gy. Gyürky, G. Imbriani, M. Junker, M. Lugaro, P. Marigo, J. Marsh, E. Masha, R. Menegazzo, D. Mercogliano, V. Paticchio, R. Perrino, P. Prati, V. Rigato, D. Robb, L. Schiavulli, R. S. Sidhu, J. Skowronski, O. Straniero, T. Szücs, S. Zavatarelli
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Abstract

The CNO cycle is one of the most important nuclear energy sources in stars. At temperatures of hydrostatic H-burning (20 MK $<$ T $<$ 80 MK) the $^{17}$O(p,$\gamma$)$^{18}$F reaction rate is dominated by the poorly constrained 64.5~keV resonance. Here we report on the first direct measurements of its resonance strength and of the direct capture contribution at 142 keV, performed with a new high sensitivity setup at LUNA. The present resonance strength of $\omega\gamma_{(p, \gamma)}$\textsuperscript{bare} = (30 $\pm$ 6\textsubscript{stat} $\pm$ 2\textsubscript{syst})~peV is about a factor of 2 higher than the values in literature, leading to a $\Gamma$\textsubscript{p}\textsuperscript{bare} = (34 $\pm$ 7\textsubscript{stat} $\pm$ 3\textsubscript{syst})~neV, in agreement with LUNA result from the (p,$\alpha$) channel. Such agreement strengthen our understanding of the oxygen isotopic ratios measured in red giant stars and in O-rich presolar grains.
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首次直接测量 $^{17}$O(p,$γ$)$^{18}$F 反应中的 64.5 keV 共振强度
在静水H燃烧的温度下(20 MK < T < 80 MK),$^{17}$O(p,$\gamma$)$^{18}$F反应速率由约束较差的64.5~keV共振所主导。在此,我们报告了利用 LUNA 的新型高灵敏度装置首次直接测量其共振强度和 142 keV 的直接俘获贡献的结果。目前的共振强度为:$omega\gamma_{(p, \gamma)}$textsupscript{bare} = (30 $\pm$6\textsubscript{stat} $\pm$ 2\textsubscript{syst})~peV ,比文献中的数值高出约2倍、从而得出$Gamma$\textsubscript{p}\textsuperscript{bare}=(34 $\pm$7\textsubscript{stat} $\pm$ 3\textsubscript{syst} )~neV,与来自(p,$\alpha$)通道的LUNA结果一致。这种一致性加强了我们对在红巨星和富氧前极粒中测得的氧同位素比值的理解。
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