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低本底高分辨测量技术在^(16)N衰变的出射α粒子测量中的应用
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作者 南威克 苏俊 +16 位作者 郭冰 谌阳平 杨彦云 王建松 许世伟 马军兵 马朋 白真 李鑫悦 韩志宇 李云居 曾晟 颜胜权 马田丽 苏毅 茹龙辉 柳卫平 《原子能科学技术》 EI CAS CSCD 北大核心 2022年第7期1230-1235,共6页
^(16)N的β延迟α衰变能谱在E_(c.m.)≈1.2 MeV处有一低能峰,该α峰的形状和高度可用于约束^(12) C(α,γ)^(16)O反应截面的E1部分,对其进行测量具有重要意义。本工作尝试采用重离子注入法对其进行测量,在兰州重离子加速器国家实验室RIB... ^(16)N的β延迟α衰变能谱在E_(c.m.)≈1.2 MeV处有一低能峰,该α峰的形状和高度可用于约束^(12) C(α,γ)^(16)O反应截面的E1部分,对其进行测量具有重要意义。本工作尝试采用重离子注入法对其进行测量,在兰州重离子加速器国家实验室RIBLL1放射性束流线上产生了^(16)N放射性束流并将其注入到双面硅微条探测器(DSSD)中,利用DSSD对其β延迟α能谱进行了测量。通过选用薄的DSSD探测器、DSSD正反面能量符合关系以及DSSD点火数约束等方法,显著减小了^(16)N衰变产生的电子对α能谱测量的干扰,将α能谱的测量阈值降低到800 keV左右,成功观测到了E_(c.m.)≈1.2 MeV处的低能峰。该方法为间接研究^(12)C(α,γ)^(16) O反应率开辟了一条新的实验方法。 展开更多
关键词 天体物理 反应率 间接测量 β延迟α能谱
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用于核天体物理实验的活性靶时间投影室 被引量:3
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作者 张志超 张宁涛 +18 位作者 鲁辰桂 蒲天磊 张金龙 陈涵 段利敏 高丙水 李阔昂 李宇田 千奕 茹龙辉 唐晓东 王新雨 徐晓栋 赵红赟 蔡紫葳 姬彬斐 李奇特 许金艳 林炜平 《原子核物理评论》 CAS CSCD 北大核心 2020年第3期636-642,共7页
发生在中子星壳层内的丰中子熔合反应对中子星演化以及X射线超级爆等现象均会产生影响。受限于放射性束流强度和反应机制的复杂性,实验数据极其缺乏,难以有效约束理论模型。基于活性靶技术的时间投影室(Time Projection Chamber,TPC)将... 发生在中子星壳层内的丰中子熔合反应对中子星演化以及X射线超级爆等现象均会产生影响。受限于放射性束流强度和反应机制的复杂性,实验数据极其缺乏,难以有效约束理论模型。基于活性靶技术的时间投影室(Time Projection Chamber,TPC)将工作气体作为反应靶,具备近4π立体角接受度和三维径迹重建能力,能够实现对反应事件的全记录,显著提高了探测效率,大幅降低了熔合反应截面测量对束流强度的要求。我们研制了240路信号读出的TPC,并使用放射性束流^(16)N对探测器进行了测试,探索了该实验方法的可行性和有效性。为了得到更加精确的反应产物径迹,对反应事件做出更好的筛选,进一步发展了1024路信号读出TPC,并开展了^(12)C+^(12)C库仑位垒附近熔合反应截面测量实验,初步实验结果与已有实验数据符合较好。 展开更多
关键词 熔合反应 活性靶 时间投影室
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Studies of the 2α and 3α channels of the ^(12)C+^(12)C reaction in the range of E_(c.m.)=8.9 MeV to 21 MeV using the active target Time Projection Chamber 被引量:4
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作者 X.Y.Wang N.T.Zhang +18 位作者 Z.C.Zhang C.G.Lu T.L.Pu J.L.Zhang L.M.Duan B.S.Gao K.A.Li Y.T.Li Y.Qian L.H.Ru B.Wang X.D.Xu H.Y.Zhao W.P.Lin Z.W.Cai B.F.Ji Q.T.Li J.Y.Xu X.D.Tang 《Chinese Physics C》 SCIE CAS CSCD 2022年第10期116-125,共10页
The ^(12)C+^(12)C fusion reaction was studied in the range of E_(c.m.)=8.9 to 21 MeV using the active-target Time Projection Chamber.With full information on all tracks of the reaction products,cross sections of the^(... The ^(12)C+^(12)C fusion reaction was studied in the range of E_(c.m.)=8.9 to 21 MeV using the active-target Time Projection Chamber.With full information on all tracks of the reaction products,cross sections of the^(12)C(^(12)C,^(8)Be)^(16)O_(g.s.)channel and the ^(12)C(^(12)C,3a)^(12)C channel could be measured down to the level of a few milibarns.The ^(12)C(^(12)C,^(8)Be)^(16)O_(g.s.)reaction channel was determined to be 10_(-8)^(+24) mb at E_(c.m.)=11.1 MeV,supporting the direct a transfer reaction mechanism.The ^(12)C(^(12)C,3α)^(12)C reaction channel was studied for the first time using an exclusive measurement.Our result does not confirm the anomaly behavior reported in the previous inclusive measurement by Kolata et al.[Phys.Rev.C 21,579(1980)].Our comparisons with statistical model calculations suggest that the 3 a channel is dominated by the fusion evaporation process at E_(c.m.)>19 MeV.The additional contribution of the 3 a channel increases the fusion reaction cross section by 10% at energies above 20 MeV.We also find that an additional reaction mechanism is needed to explain the measured cross section at E_(c.m.)<15 MeV at which point the statistical model prediction vanishes. 展开更多
关键词 fusion cross section Coulomb barrier Time Projection Chamber active target
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Modified astrophysical S-factor of 12C+12C fusion reaction at sub-barrier energies
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作者 Y.J.Li X.Fang +3 位作者 B.Bucher K.A.Li L.H.Ru X.D.Tang 《Chinese Physics C》 SCIE CAS CSCD 2020年第11期189-207,共19页
The 12C+12C fusion reaction plays a crucial role in stellar evolution and explosions.Its main open reaction channels includeα,p,n,and 8Be.Despite more than a half century of efforts,large differences remain among the... The 12C+12C fusion reaction plays a crucial role in stellar evolution and explosions.Its main open reaction channels includeα,p,n,and 8Be.Despite more than a half century of efforts,large differences remain among the experimental data of this reaction measured using various techniques.In this work,we analyze the existing data using a statistical model.Our calculation shows the following:1)the relative systematic uncertainties of the predicted branching ratios decrease as the predicted ratios increase;2)the total modified astrophysical S-factors(S^* factors)of the p andαchannels can be obtained by summing the S^* factors of their corresponding ground-state transitions and the characteristicγrays,while taking into account the contributions of the missing channels to the latter.After applying corrections based on branching ratios predicted by the statistical model,an agreement is achieved among the different data sets at Ecm>4 MeV,while some discrepancies remain at lower energies,suggesting the need for better measurements in the near future.We find that the S^* factor recently obtained from an indirect measurement is inconsistent with the direct measurement value at energies below 2.6 MeV.We recommend upper and lower limits for the 12C+12C S^* factor based on the existing models.A new 12C+12C reaction rate is also recommended. 展开更多
关键词 carbon burning 12C+12C fusion statistical model quasi-molecular resonance astrophysical S-factor reaction rate stellar evolution
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