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arXiv 1101.2632astro-ph.SR
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致密气体和流出物的性质

Dense gas and the nature of the outflows

I. Sepúlveda, G. Anglada, R. Estalella, R. López, J. M. Girart, J. Yang

摘要:

利用Haystack天文台的37 m射电望远镜观测了NH3分子的(J,K)=(1,1)和(J,K)=(2,2)反转跃迁。我们在27个观测区域检测到NH3排放,并绘制了其中25个区域的地图。此外,我们还在6个区域寻找了6{16}-5 23} H2O脉泽谱线,在其中两个区域HH 265和AFGL 5173探测到了H2O脉泽发射。我们估计NH3映射的区域的物理参数,并分析每个特定区域的高密度气体的分布及其与年轻恒星物体的存在的关系。从我们的数据的全球分析,我们发现,在一般的最高值的线宽获得的质量和动力学温度的最高值的区域。我们还发现了非热谱线宽度和辐射热光度的来源之间的相关性,以及核心的质量和辐射热光度之间的相关性。我们用更大的区域样本证实了Anglada等人(1997)的结论,即分子流出源的NH3谱线发射比光学流出源的NH3谱线发射更强,这表明了一种可能的演化方案,在这种方案中,与分子流出有关的年轻恒星物体逐渐失去其邻近的高密度气体,在此过程中削弱了NH3发射和分子流出,并且随着气体总量的减少使得光学射流更容易被检测。

英文摘要:

We present the results of the observations of the (J,K)=(1,1) and the (J,K)=(2,2) inversion transitions of the NH3 molecule toward a large sample of 40 regions with molecular or optical outflows, using the 37 m radio telescope of the Haystack Observatory. We detected NH3 emission in 27 of the observed regions, which we mapped in 25 of them. Additionally, we searched for the 6{16}-5{23} H2O maser line toward six regions, detecting H2O maser emission in two of them, HH265 and AFGL 5173. We estimate the physical parameters of the regions mapped in NH3 and analyze for each particular region the distribution of high density gas and its relationship with the presence of young stellar objects. From the global analysis of our data we find that in general the highest values of the line width are obtained for the regions with the highest values of mass and kinetic temperature. We also found a correlation between the nonthermal line width and the bolometric luminosity of the sources, and between the mass of the core and the bolometric luminosity. We confirm with a larger sample of regions the conclusion of Anglada et al. (1997) that the NH3 line emission is more intense toward molecular outflow sources than toward sources with optical outflow, suggesting a possible evolutionary scheme in which young stellar objects associated with molecular outflows progressively lose their neighboring high-density gas, weakening both the NH3 emission and the molecular outflow in the process, and making optical jets more easily detectable as the total amount of gas decreases.

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