论文标题
具有旋转VI的恒星模型的网格:型号从0.8到120 $ m_ \ odot $在金属性z = 0.006
Grids of stellar models with rotation VI: Models from 0.8 to 120 $M_\odot$ at a metallicity Z = 0.006
论文作者
论文摘要
上下文:使用相同物理成分计算的恒星模型的网格,允许人们研究给定物理对广泛初始条件的影响,并且是建模星系演变的关键成分。目的:我们为0.8至120 $ m_ \ odot $质量的单星模型呈现一个网格,其中有没有旋转的重量分数为重元z = 0.006,代表了大型麦哲伦云(LMC)。方法:我们使用了日内瓦恒星演化代码。计算演化,直到中央碳燃烧阶段的结束,早期渐近巨型分支相或分别用于大型,中间和低质量恒星的核心氦闪 - 。结果:当前恒星模型的输出由我们组在此处考虑的金属上和之下获得的两个网格的输出很好地构成。本工作的模型为LMC中恒星的主序列中观察到的氮表面富集提供了很好的拟合,其初始质量约为15 $ m_ \ odot $。他们还重现了LMC井红色超级巨人的光度函数的斜率,这是对红色超级阶段比时间平均质量损失率敏感的特征。在Z = 0.006处的本型号可以形成的最大的黑洞约为55 $ m_ \ odot $。在考虑的质量范围内,没有任何模型将进入配对的超新星制度,而对旋转模型的最小质量进入旋转型不稳定性区域约为60美元$ m_ \ odot $,对于非盘旋型号的型号为85 $ m_ \ odot $。结论:当前模型与在LMC中的观察以及在银河系外部区域的比较特别有趣。我们提供公众访问数值表,可用于计算插值轨道和人群合成研究。
Context: Grids of stellar models, computed with the same physical ingredients, allow one to study the impact of a given physics on a broad range of initial conditions and are a key ingredient for modeling the evolution of galaxies. Aims: We present a grid of single star models for masses between 0.8 and 120 $M_\odot$, with and without rotation for a mass fraction of heavy element Z=0.006, representative of the Large Magellanic Cloud (LMC). Methods: We used the Geneva stellar evolution code. The evolution was computed until the end of the central carbon-burning phase, the early asymptotic giant branch phase, or the core helium-flash for massive, intermediate, and low mass stars, respectively. Results: The outputs of the present stellar models are well framed by the outputs of the two grids obtained by our group for metallicities above and below the one considered here. The models of the present work provide a good fit to the nitrogen surface enrichments observed during the main sequence for stars in the LMC with initial masses around 15 $M_\odot$. They also reproduce the slope of the luminosity function of red supergiants of the LMC well, which is a feature that is sensitive to the time-averaged mass loss rate over the red supergiant phase. The most massive black hole that can be formed from the present models at Z=0.006 is around 55 $M_\odot$. No model in the range of mass considered will enter into the pair-instability supernova regime, while the minimal mass to enter the region of pair pulsation instability is around 60 $M_\odot$ for the rotating models and 85 $M_\odot$ for the nonrotating ones. Conclusions: The present models are of particular interest for comparisons with observations in the LMC and also in the outer regions of the Milky Way. We provide public access to numerical tables that can be used for computing interpolated tracks and for population synthesis studies.