基于密度泛函理论的热致密等离子体辐射不透明度计算模型

S. Kiyokawa
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引用次数: 0

摘要

我们通过时间依赖密度泛函理论(TDDFT)来确定局部热平衡(LTE)下等离子体的辐射不透明度,包括自电离共振,其中使用详细配置计算(DCA)方法计算嵌入等离子体中的离子的光吸收截面。利用有限温度密度泛函理论(FTDFT)确定了具有整数占位数的离子的丰度。对于温度为eV,密度为0.01 g/cm3的Al等离子体,我们得到了b-f和b-b跃迁的多普勒和Stark宽度的不透明度和光吸收截面,也得到了普朗克和Rosseland平均不透明度分别为28,348 cm2/g和4,279 cm2/g的结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Model of Calculating Radiative Opacities of Hot Dense Plasmas Based on the Density-Functional Theory
We determine the radiative opacity of plasmas in a local thermal equilibrium (LTE) by time-dependent density-functional theory (TDDFT) including autoionization resonances, where the photoabsorption cross section is calculated for an ion embedded in the plasma using the detailed configuration accounting (DCA) method. The abundance of ion with integer occupation numbers is determined by means of the finite temperature density-functional theory (FTDFT). For an Al plasma of temperature eV and density 0.01 g/cm3, we show the opacity and the photoabsorption cross section of b-f and b-b transitions with Doppler and Stark width, and also show a result that the Planck and Rosseland mean opacities are 28,348 cm2/g and 4,279 cm2/g, respectively.
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