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arXiv 0806.1877astro-ph
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Herbig Ae星HD169142周围盘中的气体和尘埃质量

Gas and dust mass in the disk around the Herbig Ae star HD169142

Olja Panić, Michiel R. Hogerheijde, David Wilner, Chunhua Qi

摘要:

本文研究了前主序星HD 169142周围盘的气体成分的物理结构。用亚毫米波列阵观测到了1.4“分辨率的~(13)CO和~(18)O J=2-1谱线发射。我们采用的磁盘物理结构来自一个模型,适合的光谱能量分布的HD 169142。我们获得了完整的三维信息的CO排放的分子激发和辐射转移代码的帮助。这些信息用于分析我们的观测和以前的12 CO J=2-1和1.3毫米连续谱数据。该磁盘是在开普勒旋转和看到的倾角接近13度从面对。我们的结论是,不同的CO同位素追踪的区域是不同的,在磁盘内的垂直位置,它们的温度和它们的柱密度。在给定的圆盘结构下,我们发现冻结不足以有效地从气相中去除大量的CO。这两条观测到的谱线在通量和排放的空间结构方面都与模型预测相匹配。因此,我们使用我们的数据来推导13 CO和C18 O的质量,并因此使用标准同位素比的12 CO质量。我们将盘上气体的总质量限制为(0.6-3.0)× 10(-2)Msun。采用每克灰尘2 cm 2的最大灰尘不透明度,我们从1.3 mm数据的拟合中得出最小灰尘质量为2.16x10(-4)Msun。通过比较得出的气体和尘埃质量表明,只有在尘埃不透明度为2 cm 2/g和12 CO相对于H2丰度为10(-4)的假设下,气体与尘埃的质量比才可能为100。然而,我们的数据也与气尘比为25、尘埃不透明度为1 cm 2/g和12 CO丰度为2x 10(-4)的情况兼容。

英文摘要:

We investigate the physical structure of the gas component of the disk around the pre-main-sequence star HD169142. The 13CO and C18O J=2-1 line emission is observed from the disk with 1.4'' resolution using the Submillimeter Array. We adopt the disk physical structure derived from a model which fits the spectral energy distribution of HD169142. We obtain the full three-dimensional information on the CO emission with the aid of a molecular excitation and radiative transfer code. This information is used for the analysis of our observations and previous 12CO J=2-1 and 1.3 mm continuum data. The disk is in Keplerian rotation and seen at an inclination close to 13 deg from face-on. We conclude that the regions traced by different CO isotopologues are distinct in terms of their vertical location within the disk, their temperature and their column densities. With the given disk structure, we find that freeze-out is not efficient enough to remove a significant amount of CO from gas phase. Both observed lines match the model prediction both in flux and in the spatial structure of the emission. Therefore we use our data to derive the 13CO and C18O mass and consequently the 12CO mass using standard isotopic ratios. We constrain the total disk gas mass to (0.6-3.0)x10(-2) Msun. Adopting a maximum dust opacity of 2 cm2 per gram of dust we derive a minimum dust mass of 2.16x10(-4) Msun from the fit to the 1.3 mm data. Comparison of the derived gas and dust mass shows that the gas to dust mass ratio of 100 is only possible under the assumption of a dust opacity of 2 cm2/g and 12CO abundance of 10(-4) with respect to H2. However, our data are also compatible with a gas to dust ratio of 25, with a dust opacity of 1 cm2/g and 12CO abundance of 2x10(-4).

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