论文标题
内星系中的Atlasgal选择的大块团块。 X.观察原子碳在492 GHz处
ATLASGAL-selected massive clumps in the inner Galaxy. X. Observations of atomic carbon at 492 GHz
论文作者
论文摘要
(删节)在本文中,我们通过分析Apex [CI] 492 GHz的Atlasgal Top100来源的Apex [CI] 492 GHz单点观测以及其他多波长数据,研究了[CI]追踪气体在高质量恒星形成区域的物理条件。在[CI] 492 GHz发射中清楚地检测到了我们的98个来源,观察到的集成强度和线宽度往往会增加到恒星形成的进化阶段。除了这些与前100个样品相关的“主要”组件外,其速度分别针对28和两条视力,将41个发射和两个吸收特征鉴定为“次级”成分。次要组件的集成强度和线宽度比主要组件具有系统较小的集成强度和线宽度。我们发现[CI] 492 GHz和13CO(2-1)与13CO(2-1) - [CI] 492 GHz综合强度比从0.2到5.3不等。此外,我们通过将870个基于微米的H2柱密度除以观察到的[CI] 492 GHz的集成强度,并发现X(CI)范围为2.3E20至1.3E22,并以1.7E21的中间值将基于[CI] 492 GHz的范围衍生出H2-to- [CI]转换因子X(CI),并发现X(CI)范围为2.3e20至1.3E22。与与13CO(2-1)的强相关性相反,[CI] 492 GHz与870微米跟踪的分子气具有散射关系。最后,我们对[CI] 492 GHz和809 GHz数据进行了LTE和非LTE分析,用于TOP100样品的一部分,并推断[CI]发射可能起源于温暖(动力学温度> 60 K),光学上较薄(不透明度<0.5),并且高压〜E5至E5至E8 K/CM3)区域。
(Abridged) In this paper, we investigate the physical conditions of [CI]-traced gas in high-mass star-forming regions by analyzing APEX [CI] 492 GHz single-pointing observations of the ATLASGAL Top100 sources along with other multi-wavelength data. Our 98 sources are clearly detected in [CI] 492 GHz emission, and the observed integrated intensities and line widths tend to increase toward evolved stages of star formation. In addition to these "main" components that are associated with the Top100 sample, 41 emission and two absorption features are identified by their velocities toward 28 and two lines of sight respectively as "secondary" components. The secondary components have systematically smaller integrated intensities and line widths than the main components. We found that [CI] 492 GHz and 13CO(2-1) are well correlated with the 13CO(2-1)-to-[CI] 492 GHz integrated intensity ratio varying from 0.2 to 5.3. In addition, we derived the H2-to-[CI] conversion factor, X(CI), by dividing 870 micron-based H2 column densities by the observed [CI] 492 GHz integrated intensities and found that X(CI) ranges from 2.3e20 to 1.3e22 with a median of 1.7e21. In contrast to the strong correlation with 13CO(2-1), [CI] 492 GHz has a scattered relation with the 870 micron-traced molecular gas. Finally, we performed LTE and non-LTE analyses of the [CI] 492 GHz and 809 GHz data for a subset of the Top100 sample and inferred that [CI] emission likely originates from warm (kinetic temperature > 60 K), optically thin (opacity < 0.5), and highly pressurized (thermal pressure ~ e5 to e8 K/cm3) regions.