论文标题
强烈磁性AP恒星HD166473的异常大气结构
The anomalous atmospheric structure of the strongly magnetic Ap star HD166473
论文作者
论文摘要
强烈磁性的,超高旋转的迅速振荡AP星HD166473的高分辨率光谱观测用于研究可变强磁场对各种化学元件的垂直和表面水平分布的存在的含义。对计算出的LSD Stokes $ i $和$ v $配置文件的分析证实了先前报道的几种化学元素的不均匀水平表面分布的检测。为了测试铁峰和稀土元素的垂直丰度分层,使用属于中性和离子化阶段的这些元素的光谱线进行了磁场测量。我们发现清楚地表明磁场强度与其方向和垂直元件之间存在关系:在接近磁性赤道的不同阶段获得的元素获得的磁场值相当相似,而在接近磁场极点的区域中,田间强度的分散体非常大。在负极和正极的阶段,根据REE线分析确定的平均纵向场强度通常比使用Fe和Cr时强。最强大的平均纵向磁场,最高为$ -4160 $ \ pm $ 226 g,使用LAI II线列表检测到负极极端列表,然后使用$ \ langle b_z \ rangle $ = $ = $ = $ -3740 $ 3740 $ \ pm $ 343 g和$ 343 g和$ 343 g和$ 343 g的pr iii行进行测量。 \ rangle $ = $ - $ 3372 $ \ pm $ 247 g。使用PR III线的最强平均平均纵向磁场,高达3584 $ \ pm $ 354 g,随后是测量$ \ langle b_z \ langle b_z \ langle b_z \ rangle $ = 2517 $ \ pm pm $ \ pm $ 249 g使用CE II行。
High resolution spectropolarimetric observations of the strongly magnetic, super-slowly rotating rapidly oscillating Ap star HD166473 are used to investigate the implications of the presence of a variable strong magnetic field on the vertical and surface horizontal distribution of various chemical elements. The analysis of the calculated LSD Stokes $I$ and $V$ profiles confirms the previously reported detection of non-uniform horizontal surface distribution of several chemical elements. To test the vertical abundance stratification of iron peak and rare earth elements, magnetic field measurements were carried out using spectral lines of these elements belonging to neutral and ionised stages. We find clear indication of the existence of a relation between the magnetic field strength and its orientation and vertical element stratification: magnetic field values obtained for elements in different stages close to the magnetic equator are rather similar whereas the dispersion in field strengths is remarkably large in the regions close to magnetic field poles. At the phases of negative and positive extrema the mean longitudinal field strength determined from the analysis of the REE lines is usually stronger than when using Fe and Cr. The strongest mean longitudinal magnetic field, up to $-$4160$\pm$226 G, is detected using the La II line list at the negative extremum, followed by the measurements using the Pr III lines with $\langle B_z \rangle$=$-$3740$\pm$343 G and the Ce II lines with $\langle B_z \rangle$=$-$3372$\pm$247 G. The strongest mean longitudinal magnetic field of positive polarity, up to 3584$\pm$354 G is detected using the Pr III lines, followed by the measurement $\langle B_z \rangle$=2517$\pm$249 G using the Ce II lines.