Gao B, Jiao T Y, Li Y T, Chen H, Lin W P, An Z, Ru L H, Zhang Z C, Tang X D, Wang X Y, Zhang N T, Fang X, Xie D H, Fan Y H, Ma L, Zhang X, Bai F, Wang P, Fan Y X, Liu G, Huang H X, Wu Q, Zhu Y B, Chai J L, Li J Q, Sun L T, Wang S, Cai J W, Li Y Z, Su J, Zhang H, Li Z H, Li Y J, Li E T, Chen C, Shen Y P, Lian G, Guo B, Li X Y, Zhang L Y, He J J, Sheng Y D, Chen Y J, Wang L H, Zhang L, Cao F Q, Nan W, Nan W K, Li G X, Song N, Cui B Q, Chen L H, Ma R G, Zhang Z C, Yan S Q, Liao J H, Wang Y B, Zeng S, Nan D, Fan Q W, Qi N C, Sun W L, Guo X Y, Zhang P, Chen Y H, Zhou Y, Zhou J F, He J R, Shang C S, Li M C, Kubono S, Liu W P, deBoer R J, Wiescher M, Pignatari M
Center for Nuclear Study, University of Tokyo, Wako, Saitama 351-0198, Japan.
Wolfson Fellow of Royal Society, School of Physics and Astronomy, University of Edinburgh, King's Buildings, Edinburgh EH9 3FD, United Kingdom.
Phys Rev Lett. 2022 Sep 23;129(13):132701. doi: 10.1103/PhysRevLett.129.132701.
The ^{13}C(α,n)^{16}O reaction is the main neutron source for the slow-neutron-capture process in asymptotic giant branch stars and for the intermediate process. Direct measurements at astrophysical energies in above-ground laboratories are hindered by the extremely small cross sections and vast cosmic-ray-induced background. We performed the first consistent direct measurement in the range of E_{c.m.}=0.24 to 1.9 MeV using the accelerators at the China Jinping Underground Laboratory and Sichuan University. Our measurement covers almost the entire intermediate process Gamow window in which the large uncertainty of the previous experiments has been reduced from 60% down to 15%, eliminates the large systematic uncertainty in the extrapolation arising from the inconsistency of existing datasets, and provides a more reliable reaction rate for the studies of the slow-neutron-capture and intermediate processes along with the first direct determination of the alpha strength for the near-threshold state.
(^{13}C(α,n)^{16}O)反应是渐近巨星分支恒星中慢中子俘获过程以及中间过程的主要中子源。由于截面极小且宇宙射线诱发的本底巨大,在地面实验室对天体物理能量下的该反应进行直接测量受到阻碍。我们利用中国锦屏地下实验室和四川大学的加速器,在质心能量(E_{c.m.}=0.24)至(1.9)兆电子伏范围内进行了首次连贯的直接测量。我们的测量几乎覆盖了整个中间过程伽莫夫窗,在此过程中,先前实验的巨大不确定性已从(60%)降至(15%),消除了因现有数据集不一致而在外推过程中产生的巨大系统不确定性,并为慢中子俘获和中间过程的研究提供了更可靠的反应速率,同时首次直接测定了近阈态的α强度。