首页> 外文期刊>The Astrophysical journal >DENSE CLUMPS IN GIANT MOLECULAR CLOUDS IN THE LARGE MAGELLANIC CLOUD: DENSITY AND TEMPERATURE DERIVED FROM 13CO(J = 3-2) OBSERVATIONS
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DENSE CLUMPS IN GIANT MOLECULAR CLOUDS IN THE LARGE MAGELLANIC CLOUD: DENSITY AND TEMPERATURE DERIVED FROM 13CO(J = 3-2) OBSERVATIONS

机译:大型麦哲伦云中巨大分子云的密集簇:从13CO(J = 3-2)观察得出的密度和温度

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In order to precisely determine the temperature and density of molecular gas in the Large Magellanic Cloud, we made observations of the optically thin 13CO(J = 3-2) transition using the ASTE 10 m telescope toward nine peaks where 12CO(J = 3-2) clumps were previously detected with the same telescope. The molecular clumps include those in giant molecular cloud (GMC) Types I (with no signs of massive star formation), II (with H II regions only), and III (with H II regions and young star clusters). We detected 13CO(J = 3-2) emission toward all the peaks and found that their intensities are 3-12 times lower than those of 12CO(J = 3-2). We determined the intensity ratios of 12CO(J = 3-2) to 13CO(J = 3-2), R 12/13 3-2, and 13CO(J = 3-2) to 13CO(J = 1-0), R 13 3-2/1-0, at 45'' resolution. These ratios were used in radiative transfer calculations in order to estimate the temperature and density of the clumps. The clumps have a kinetic temperature range of T kin = 15-200?K and a molecular hydrogen gas density range of n(H2) = 8 × 102-7 × 103?cm–3. We confirmed that the higher density clumps have higher kinetic temperature and that the lower density clumps have lower kinetic temperature to better accuracy than in previous work. The kinetic temperature and density increase generally from a Type I GMC to a Type III GMC. We interpret that this difference reflects an evolutionary trend of star formation in molecular clumps. The R 13 3-2/1-0 and kinetic temperature of the clumps are well correlated with the Hα flux, suggesting that the heating of molecular gas with density n(H2) = 103-104?cm–3 can be explained by stellar far-ultravoilet photons.
机译:为了精确确定大麦哲伦星云中分子气体的温度和密度,我们使用ASTE 10 m望远镜观察了光学上稀薄的13CO(J = 3-2)跃迁到9个峰的位置,其中12CO(J = 3 2)以前使用同一望远镜检测到团块。分子团块包括I型(没有大质量恒星形成迹象),II型(仅具有H II区)和III型(具有H II区和年轻恒星团)的巨分子云。我们检测到所有峰的13CO(J = 3-2)发射,发现它们的强度比12CO(J = 3-2)的强度低3-12倍。我们确定了12CO(J = 3-2)与13CO(J = 3-2),R 12/13 3-2和13CO(J = 3-2)与13CO(J = 1-0)的强度比R 13 3-2 / 1-0,分辨率为45英寸。这些比率用于辐射传递计算中,以估算团块的温度和密度。团块的动态温度范围为T kin = 15-200?K,分子氢气浓度范围为n(H2)= 8×102-7×103?cm–3。我们证实,与以前的工作相比,较高密度的团块具有较高的动力学温度,较低密度的团块具有较低的动力学温度。动力学温度和密度通常从I型GMC升高到III型GMC。我们解释说,这种差异反映了分子团块中恒星形成的演化趋势。 R 13 3-2 / 1-0和团块的动力学温度与Hα通量密切相关,这表明恒星可以解释密度为n(H2)= 103-104?cm–3的分子气体的加热远紫外光子。
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