首页> 外文期刊>The Astrophysical journal >CROSS SECTION FOR THE ASTROPHYSICAL ~(14)C(n, γ)~(15)C REACTION VIA THE INVERSE REACTION
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CROSS SECTION FOR THE ASTROPHYSICAL ~(14)C(n, γ)~(15)C REACTION VIA THE INVERSE REACTION

机译:〜(14)C(n,γ)〜(15)C反应的天体物理截面

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摘要

The ~(14)C(n, γ)~(15)C reaction is important in neutron-induced CNO cycles of stellar evolution phases beyond the main sequence. The chain of reactions in primordial nucleosynthesis in the neutron-rich environment of an inhomogeneous big bang also involves the ~(14)C(n, γ)~(15)C reaction. We have used a beam of ~(15)C ions at E/A = 35 MeV to measure cross sections for ~(15)C breakup on targets of C, Al, Zn, Sn, and Pb. The Coulomb part of the breakup cross section was determined as a function of decay energy. By the principle of detailed balance, the neutron capture cross section was then determined as a function of neutron energy. This excitation function rises with energy to 7 μbarns at 300 keV and falls to 2 μbarns at 1.2 MeV. In the stellar-burning region, our cross section exceeds a previous measurement by a factor of 3. Neither the shape nor the magnitude of the excitation function agrees with those of theoretical calculations based on the direct capture model. The reaction rate is calculated reliably up to ~T_9 = 5. In the temperature range of inhomogeneous big bang models, our rate exceeds the rate of the ~(14)C(p, γ)~(15)N reaction for T_9 < 1.2.
机译:〜(14)C(n,γ)〜(15)C反应在中子诱发的,超出主要序列的恒星演化阶段的CNO循环中很重要。在不均匀大爆炸的富中子环境中,原始核合成中的反应链也涉及〜(14)C(n,γ)〜(15)C反应。我们已使用E / A = 35 MeV的〜(15)C离子束来测量C,Al,Zn,Sn和Pb靶上〜(15)C分解的截面。确定破裂横截面的库仑部分作为衰变能量的函数。根据详细平衡原理,然后确定中子俘获截面与中子能量的关系。该激发函数在300 keV时随能量上升至7μbarns,在1.2 MeV时下降至2μbarns。在恒星燃烧区域,我们的横截面比以前的测量值大3倍。激励函数的形状和大小都与基于直接捕获模型的理论计算结果不一致。可靠地计算出反应速率,直到〜T_9 =5。在不均匀大爆炸模型的温度范围内,我们的速率超过了T_9 <1.2时〜(14)C(p,γ)〜(15)N反应的速率。 。

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