$^{157,159}$Ho和$^{163,165}$Tm的光核反应速率及其在$γ$--过程中的影响

Hao Cheng, Bao-Hua Sun, Li-Hua Zhu, Motohiko Kusakabe, Yudong Luo, Toshitaka Kajino, Chang-Jian Wang, Xing-Qun Yao, Chuang-Ye He, Fu-Long Liu, Bing Guo
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摘要

恒星条件下可靠的光核反应率对于了解介于$^{74}$Se和$^{196}$Hg-p-核之间的重稳定中子缺失同位素的起源至关重要,然而,由于实验进展稀少,许多相关的反应率仍然不得不依赖于豪瑟-费斯巴赫模型。Dy、Er、Ho 和 Tmisotopes 的质量范围为 160 就是这样一种情况。在这项工作中,我们试图通过再现$^{160}$Dy($p,\gamma$)$^{161}$Ho和$^{162}$Er($p,\gamma$)$^{163}$Tm在$A/sim 160$质量区的现有实验数据,来约束TALYS软件包中的豪瑟-费斯巴赫模型,并检验水平密度、伽马强度函数和光学模型势的影响。受约束的模型允许我们计算$^{157, 159}$Ho($\gamma$, $p$)和$^{163,165}$Tm($\gamma$, $p$)的反应速率,以用于$\gamma$过程核合成中的碳-脱燃SNE Ia模型。在2-3 GK的温度范围内,我们推荐的速率与JINAREACLIB相差1个数量级以上。这导致在$A\sim 160$质量范围内,$p$核的最终丰度与JINA的相比发生了-5.5-3%的变化,这意味着($\gamma$,$p$)反应的不确定性在核的合成中并不占主导地位。
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Photo-nuclear reaction rates of $^{157,159}$Ho and $^{163,165}$Tm and their impact in the $γ$--process
Reliable photo-nuclear reaction rates at the stellar conditions are essential to understand the origin of the heavy stable neutron-deficient isotopes between $^{74}$Se and $^{196}$Hg-p-nuclei, however, many reaction rates of relevance still have to rely on the Hauser-Feshbach model due to rare experimental progress. One such case is in the mass range of 160 for Dy, Er, Ho and Tm isotopes. In this work we attempt to constrain the Hauser-Feshbach model in the TALYS package by reproducing the available experimental data of $^{160}$Dy($p,\gamma$)$^{161}$Ho and $^{162}$Er($p,\gamma$)$^{163}$Tm in the $A\sim 160$ mass region, and examine the effects of level density, gamma strength function and the optical model potential. The constrained model then allows us to calculate the reaction rates of $^{157, 159}$Ho($\gamma$, $p$) and $^{163,165}$Tm($\gamma$, $p$) for the $\gamma$-process nucleosynthesis in carbon-deflagration SNe Ia model. Our recommended rates differ from the JINA REACLIB by more than 1 order of magnitude in the temperature range of 2-3 GK. This results in the changes of final abundance of $p$-nuclei in the $A\sim 160$ mass range by -5.5-3\% from those with JINA, which means that the ($\gamma$, $p$) reactions uncertainty is not predominant for the synthesis of these nuclei.
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