论文标题
来自高分辨率光学和近红外卡门光谱的FGK型星的恒星大气参数
Stellar atmospheric parameters of FGK-type stars from high-resolution optical and near-infrared CARMENES spectra
论文作者
论文摘要
为了评估近红外波长区域高分辨率和高信噪比光谱的经典光谱方法,我们选择了65个F-,G-和K型星的样品,该样品使用Carmenes,新型,超稳定的,双稳定的,双稳定的,双渠道光谱仪观察到3.5 M Calar Alto telescope。我们通过Stepar Code(使用Stepar Code,一种拼图实现了2017版的Moog代码和Marcs模型的网格MARCS MALDERES的网格。我们编制了四个Fe I和Fe II线列表,这些列表适合于金属富含金属的矮人,金属贫困矮人,富含金属的巨人和金属贫困巨头,覆盖波长范围为5300到17100埃17100埃词,因此大大增加了已确定的FE I和FE II和FE II和Fe II和FE II和Fe II和23和23条的数量。我们检查了详尽的文献搜索后,近红外Fe I和Fe II线对我们的参数确定的影响,特别强调了我们样本中包含的14 $ GAIA $基准星。即使我们的参数确定与文献值保持良好的一致性,当考虑到近红外区域时,Fe I和Fe II线的数量的增加表明,更深的$ t _ {\ rm eff} $刻度可能源于近frared线上对$ t _ {\ rm t_ {\ rm rm aff} $的较高敏感性。
With the purpose of assessing classic spectroscopic methods on high-resolution and high signal-to-noise ratio spectra in the near-infrared wavelength region, we selected a sample of 65 F-, G-, and K-type stars observed with CARMENES, the new, ultra-stable, double-channel spectrograph at the 3.5 m Calar Alto telescope. We computed their stellar atmospheric parameters ($T_{\rm eff}$, $\log{g}$, $ξ$, and [Fe/H]) by means of the StePar code, a Python implementation of the equivalent width method that employs the 2017 version of the MOOG code and a grid of MARCS model atmospheres. We compiled four Fe I and Fe II line lists suited to metal-rich dwarfs, metal-poor dwarfs, metal-rich giants, and metal-poor giants that cover the wavelength range from 5300 to 17100 angstroms, thus substantially increasing the number of identified Fe I and Fe II lines up to 653 and 23, respectively. We examined the impact of the near-infrared Fe I and Fe II lines upon our parameter determinations after an exhaustive literature search, placing special emphasis on the 14 $Gaia$ benchmark stars contained in our sample. Even though our parameter determinations remain in good agreement with the literature values, the increase in the number of Fe I and Fe II lines when the near-infrared region is taken into account reveals a deeper $T_{\rm eff}$ scale that might stem from a higher sensitivity of the near-infrared lines to $T_{\rm eff}$.