恒星环境中原子核上的电子俘获

P. Giannaka, T. Kosmas
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引用次数: 0

摘要

原子核上的恒星电子捕获是一个重要的半轻子过程,在核心坍缩超新星的中心环境和爆炸恒星核合成中尤为重要。在这篇文章中,基于我们在之前的工作中计算的一组中等质量核同位素在实验室条件下的原始(绝对)电子捕获截面,我们扩展了这项研究并评估了恒星环境下的折叠电子捕获率。基于这一目的,我们假设母核和抛射电子在大质量恒星演化的后期阶段处于恒星内部深处时会发生相互作用。在这些条件下(超新星前阶段和核心坍缩超新星阶段的高物质密度和高温),我们选择了两类核;第一种是含有A65的48Ti和56Fe同位素。在前者中,电子捕获主要发生在前超新星阶段,而后者发生在核心坍缩超新星阶段。还包括与以前计算的比较,这些计算是通过使用用于单电荷交换核反应的各种微观核模型获得的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron Capture on Nuclei in Stellar Environment
The stellar electron capture on nuclei is an essential, semi-leptonic process that is especially significant in the central environment of core-collapse supernovae and in the explosive stellar nucleosynthesis. In this article, on the basis of the original (absolute) electron-capture cross-sections under laboratory conditions that we computed in our previous work for a set of medium-weight nuclear isotopes, we extend this study and evaluate folded e−-capture rates in the stellar environment. With this aim, we assume that the parent nuclei and the projectile electrons interact when they are in the deep stellar interior during the late stages of the evolution of massive stars. Under these conditions (high matter densities and high temperatures of the pre-supernova and core-collapse supernova phases), we choose two categories of nuclei; the first includes the 48Ti and 56Fe isotopes that have A<65 and belong to the iron group of nuclei, and the second includes the heavier and more neutron-rich isotopes 66Zn and 90Zr (with A>65). In the former, the electron capture takes place mostly during the pre-supernova stage, while the latter occurs during the core-collapse supernova phase. A comparison with previous calculations, which were obtained by using various microscopic nuclear models employed for single-charge exchange nuclear reactions, is also included.
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