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Influence of inelastic collisions with hydrogen atoms on the non-local thermodynamic equilibrium line formation for Fe? I and Fe? II in the 1D model atmospheres of late-type stars

机译:与氢原子的非弹性碰撞对Fe?的非局部热力学平衡线形成的影响 I 和Fe? II 在晚型恒星的一维模型大气中

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Context. Iron plays a crucial role in studies of late-type stars. In their atmospheres, neutral iron is the minority species, and lines of Fe? I are subject to the departures from local thermodynamic equilibrium (LTE). In contrast, one believes that LTE is a realistic approximation for Fe? II lines. The main source of the uncertainties in the non-LTE (NLTE) calculations for cool atmospheres is a treatment of inelastic collisions with hydrogen atoms. Aims. Our aim is to investigate the effect of Fe? I + H? I and Fe? II + H? I collisions and their different treatments on the Fe? I /Fe? II ionisation equilibrium and iron abundance determinations for three Galactic halo benchmark stars (HD 84937, HD 122563, and HD 140283) and a sample of 38 very metal-poor giants in the dwarf galaxies with well known distances. Methods. We performed the NLTE calculations for Fe? I –Fe? II by applying quantum-mechanical rate coefficients for collisions with H? I from recent papers. Results. We find that collisions with H? I serve as efficient thermalisation processes for Fe? II , to an extent that the NLTE abundance corrections for Fe? II lines do not exceed 0.02 dex, in absolute value, for [Fe/H] ??3, and reach +0.06 dex at [Fe/H] ~?4. For a given star, different treatments of Fe? I + H? I collisions lead to similar average NLTE abundances from the Fe? I lines, although discrepancies in the NLTE abundance corrections exist for individual lines. By using quantum-mechanical collisional data and the Gaia -based surface gravity, we obtain consistent abundances from the two ionisation stages, Fe? I and Fe? II , for red giant HD 122563. For turn-off star HD 84937, and subgiant HD 140283, we analyse the iron lines in the visible and the ultra-violet (UV, 1968–2990 ?) ranges. For either Fe? I or Fe? II , abundances from the visible and UV lines are found to be consistent in each star. The NLTE abundances from the two ionisation stages agree within 0.10 dex and 0.13 dex for two different treatments of Fe? I + H? I collisions. The Fe? I /Fe? II ionisation equilibrium is achieved for each star of our stellar sample in the dwarf galaxies, with the exception of stars at [Fe/H] ??3.7.
机译:上下文。铁在晚型恒星的研究中起着至关重要的作用。在他们的大气中,中性铁是少数物种,而铁系是铁?我受制于局部热力学平衡(LTE)。相反,有人认为LTE是Fe?的现实近似。 II线。非LTE(NLTE)计算中的冷空气不确定性的主要来源是与氢原子的非弹性碰撞的处理。目的我们的目的是研究铁的作用?我+ H?我和铁? II + H?我对铁的碰撞及其不同的处理方式?我/ Fe?对三个银河晕基准星(HD 84937,HD 122563和HD 140283)以及矮星系中38个金属贫乏的巨星(具有已知距离)进行II电离平衡和铁丰度测定。方法。我们对铁进行了NLTE计算?我-铁? II通过应用量子力学速率系数来与H 2碰撞。我来自最近的论文。结果。我们发现与H的碰撞?我可以作为Fe的有效热化工艺吗? II,在某种程度上,NLTE对Fe的丰度校正?对于[Fe / H] 3,II线绝对值不超过0.02 dex,在[Fe / H]〜4时达到+0.06 dex。对于给定的恒星,铁的不同处理方式?我+ H?我的碰撞会导致Fe产生类似的平均NLTE丰度吗? I行,尽管个别行存在NLTE丰度校正中的差异。通过使用量子力学碰撞数据和基于Gaia的表面重力,我们从两个电离阶段Fe?2获得了一致的丰度。我和铁? II,红色巨型HD122563。对于关闭恒星HD 84937和次要HD 140283,我们分析了可见光和紫外线(UV,1968–2990年)范围内的铁线。对于铁?我还是铁? II,发现可见和紫外线线的丰度在每颗恒星中是一致的。对于两种不同的Fe 2+处理,两个电离阶段的NLTE丰度在0.10 dex和0.13 dex之间。我+ H?我撞了铁?我/ Fe?除矮星系中[Fe / H]≥3.7的恒星外,矮星系中每个恒星样本的恒星均实现了II电离平衡。

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