论文标题
太阳光球硅的丰度根据CO5Bold:研究线扩展,磁场和模型效应
The solar photospheric silicon abundance according to CO5BOLD: Investigating line broadening, magnetic fields, and model effects
论文作者
论文摘要
在这项工作中,我们提出了使用Co5bold模型大气和Linfor3D光谱合成代码得出的光球太阳硅丰度。以前的工作在选择光谱线样本和模型大气以及对观察材料的处理方面有所不同,近年来太阳硅丰度经历了下降的修订。我们还显示了所选的线样本的影响,由于速度场,碰撞扩展,模型空间分辨率和磁场而拓宽。太阳的CO5bold模型大气与Linfor3D光谱合成代码结合使用,以生成模型光谱,然后将其适合于汉堡太阳能地图集中的观测。我们提供了在光学和红外线中的11条精心选择的线的样本(从最初选择的39行选择),并以新确定的振荡器强度适合大多数这些线。我们的最终样本包括七个光学SI I线,三个红外线线和一条光学SI II线。我们得出了$ \logε_\ mathrm {si} = 7.57 \ pm 0.04 $的光电太阳能硅丰度,其中包括$ -0.01 $ dex从非本地热力学平衡(NLTE)效果。将其与陨石丰度和先前确定的光谱丰度相结合会导致金属质量分数z/x = $ 0.0220 \ pm 0.0020 $。我们发现获得过度宽的合成线的趋势。我们通过设计除法程序来减轻这种影响。综合线的过度延伸并没有基本影响最终确定的丰度。主要是线路选择会影响最终拟合的丰度。
In this work, we present a photospheric solar silicon abundance derived using CO5BOLD model atmospheres and the LINFOR3D spectral synthesis code. Previous works have differed in their choice of a spectral line sample and model atmosphere as well as their treatment of observational material, and the solar silicon abundance has undergone a downward revision in recent years. We additionally show the effects of the chosen line sample, broadening due to velocity fields, collisional broadening, model spatial resolution, and magnetic fields. CO5BOLD model atmospheres for the Sun were used in conjunction with the LINFOR3D spectral synthesis code to generate model spectra, which were then fit to observations in the Hamburg solar atlas. We present a sample of 11 carefully selected lines (from an initial choice of 39 lines) in the optical and infrared, made possible with newly determined oscillator strengths for the majority of these lines. Our final sample includes seven optical Si I lines, three infrared Si I lines, and one optical Si II line. We derived a photospheric solar silicon abundance of $\log ε_\mathrm{Si} = 7.57 \pm 0.04$, including a $-0.01$ dex correction from Non-Local Thermodynamic Equilibrium (NLTE) effects. Combining this with meteoritic abundances and previously determined photospheric abundances results in a metal mass fraction Z/X = $0.0220 \pm 0.0020$. We found a tendency of obtaining overly broad synthetic lines. We mitigated the impact of this by devising a de-broadening procedure. The over-broadening of synthetic lines does not substantially affect the abundance determined in the end. It is primarily the line selection that affects the final fitted abundance.