GUO Bing, LI Zhi-hong, M. Lugaro, J. Buntain, PANG Dan-yang, LI Yun-ju, SU Jun, YAN Sheng-quan, WU Zhi-dan, BAI Xi-xiang, CHEN Yong-shou, DU Xian-chao, FAN Qi-wen, GAN Lin, JIN Sun-jun, A. I. Karakas, LI Er-tao, LI Zhi-chang, LIAN Gang, LIU Jian-cheng, LIU Xin, SHI Jian-rong, SHU Neng-chuan, WANG Bao-xiang, WANG You-bao, ZENG Sheng, LIU Wei-ping. Study of Neutron Source Reaction 13C(α,n)16O in Stars[J]. Atomic Energy Science and Technology, 2014, 48(2): 193-200. DOI: 10.7538/yzk.2014.48.02.0193
Citation: GUO Bing, LI Zhi-hong, M. Lugaro, J. Buntain, PANG Dan-yang, LI Yun-ju, SU Jun, YAN Sheng-quan, WU Zhi-dan, BAI Xi-xiang, CHEN Yong-shou, DU Xian-chao, FAN Qi-wen, GAN Lin, JIN Sun-jun, A. I. Karakas, LI Er-tao, LI Zhi-chang, LIAN Gang, LIU Jian-cheng, LIU Xin, SHI Jian-rong, SHU Neng-chuan, WANG Bao-xiang, WANG You-bao, ZENG Sheng, LIU Wei-ping. Study of Neutron Source Reaction 13C(α,n)16O in Stars[J]. Atomic Energy Science and Technology, 2014, 48(2): 193-200. DOI: 10.7538/yzk.2014.48.02.0193
  • 13C(α,n)16O is the main neutron source reaction of slow neutron capture (s) process in asymptotic giant branch (AGB) stars. The 6.356 MeV 1/2+ subthreshold resonance in 17O plays an important role in the 13C(α,n)16O reaction. The 13C(11B, 7Li)17O angular distributions were measured using HI-13 tandem accelerator and Q3D magnetic spectrograph, and then used to determine the α-width of the subthreshold resonant state which is currently the most uncertain parameter for determining the 13C(α,n)16O reaction rate. By using the present α-width, the astrophysical S-factor and the stellar rate of the 13C(α,n)16O reaction were derived. This shed some light on the existing discrepancies up to a factor of 25 in S-factors derived from different authors. The simulation of s-process in AGB stars shows that the new reaction rate produces 25% more Pb than the CF88 compilation.
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