Measurement of the 18 O( α , γ ) 22 Ne resonances at JUNA

22 Ne( α , n ) 25 Mg is one of the main neutron sources of the s process. 22 Ne is produced by the 14 N( α , γ ) 18 F( β + ) 18 O( α , γ ) 22 Ne reaction chain in the helium burning, thus, the production rate of 22 Ne is dominated by 14 N( α , γ ) 18 F and 18 O( α , γ ) 22 Ne. At the astrophysical r...

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Veröffentlicht in:EPJ Web of conferences 2022, Vol.260, p.11015
Hauptverfasser: Wang, Luohuan, Su, Jun, Shen, Yangping, He, Jianjun, Zhang, Liyong, Li, Xinyue, Lian, Gang, Guo, Bing, Sheng, Yaode, Chen, Yinji, Zhang, Hao, Li, Ziming, Song, Luyang, Jiang, Xinzhi, Nan, Wei, Nan, Weike, Zhang, Long, Cao, Fuqiang, Liu, Weiping
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Sprache:eng
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Zusammenfassung:22 Ne( α , n ) 25 Mg is one of the main neutron sources of the s process. 22 Ne is produced by the 14 N( α , γ ) 18 F( β + ) 18 O( α , γ ) 22 Ne reaction chain in the helium burning, thus, the production rate of 22 Ne is dominated by 14 N( α , γ ) 18 F and 18 O( α , γ ) 22 Ne. At the astrophysical relevant temperatures, the 18 O( α , γ ) 22 Ne reaction rates are determined by several low-energy resonances. In this work, the 18 O( α , γ ) 22 Ne reaction was measured at the 400 kV accelerator of Jinping Underground Nuclear Astrophysics experiment (JUNA). The γ -ray yields of the resonances between 470 to 770 keV were obtained.
ISSN:2100-014X
2100-014X
DOI:10.1051/epjconf/202226011015