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arXiv 1009.3175astro-ph.SR
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核心坍缩超新星中Ti44和Ni56的变化趋势

Trends in Ti44 and Ni56 from Core-Collapse Supernovae

Georgios Magkotsios, Francis X. Timmes, Aimee L. Hungerford, Christopher L. Fryer, Patrick A. Young, Michael Wiescher

摘要:

我们比较了从后处理的热力学轨迹从三个不同的核心崩溃模型-仙后座A祖,双冲击超新星祖,和旋转的2D爆炸-从指数和幂律轨迹的产量的钛44和镍56的产量。在这些核心塌陷模型中实现的峰值温度和密度跨越了我们确定的几个不同的核合成区域,导致不同质量元素的Ti 44和Ni 56产率有不同的趋势。指数和幂律曲线的Ti 44和Ni 56质量分数曲线通常解释了后处理产率的趋势,这取决于模型遍历的区域。我们发现,从指数和幂律轨迹的Ti 44和Ni 56的综合收益率一般是在一个因素2或更少的后处理产量。我们还分析了特定的核反应对Ti 44和Ni 56丰度演化的影响。在全球范围内影响所有产率的反应是3a,p(e-,nu)n和n(e+,nubar)p。其余反应根据其对Ti 44合成的影响程度进行排名。主要的反应包括Ti 44(a,p)V 47、Ca 40(a,g)Ti 44、V 45(p,g)Cr 46、Ca 40(a,p)Sc 43、F17(a,p)Ne 20、Na 21(a,p)Mg 24、Sc 41(p,g)Ti 42、Sc 43(p,g)Ti 44、Ti 44(p,g)V 45和Ni 57(p,g)Cu 58,以及许多弱反应。我们的分析表明,并不是所有的钛44需要产生在一个丰富的冻结出核心崩溃事件,并结合时间尺度效应的膨胀配置文件的反应速率平衡可以解释在超新星遗迹中观察到的钛44的缺乏。

英文摘要:

We compare the yields of Ti44 and Ni56 produced from post-processing the thermodynamic trajectories from three different core-collapse models -- a Cassiopeia A progenitor, a double shock hypernova progenitor, and a rotating 2D explosion -- with the yields from exponential and power-law trajectories. The peak temperatures and densities achieved in these core-collapse models span several of the distinct nucleosynthesis regions we identify, resulting in different trends in the Ti44 and Ni56 yields for different mass elements. The Ti44 and Ni56 mass fraction profiles from the exponential and power-law profiles generally explain the tendencies of the post-processed yields, depending on which regions are traversed by the model. We find integrated yields of Ti44 and Ni56 from the exponential and power-law trajectories are generally within a factor 2 or less of the post-process yields. We also analyze the influence of specific nuclear reactions on the Ti44 and Ni56 abundance evolution. Reactions that affect all yields globally are the 3a, p(e-,nu)n and n(e+,nubar)p. The rest of the reactions are ranked according to their degree of impact on the synthesis of Ti44. The primary ones include Ti44(a,p)V47, Ca40(a,g)Ti44, V45(p,g)Cr46, Ca40(a,p)Sc43, F17(a,p)Ne20, Na21(a,p)Mg24, Sc41(p,g)Ti42, Sc43(p,g)Ti44, Ti44(p,g)V45, and Ni57(p,g)Cu58, along with numerous weak reactions. Our analysis suggests that not all Ti44 need be produced in an a-rich freeze-out in core-collapse events, and that reaction rate equilibria in combination with timescale effects for the expansion profile may account for the paucity of Ti44 observed in supernovae remnants.

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