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Tracing the shock precursors in the L1448-mm/IRS3 outflows

机译:追踪L1448-mm / IRS3流出中的冲击前体

摘要

We present the detection of the SiO v=0 J=2-1 and J=3-2 lines, and of the HCO 101-000 J=3/2-1/2 F=2-1 line at ambient velocities towards the molecular outflows in L1448-mm and L1448-IRS3. This is the first detection of HCO in a dark cloud. We have also measured lines of H13CO+, H13CN, HN13C, CH3OH, and N2H+. While the HCO and the SiO lines have the narrowest profiles with linewidths of 0.5 km s-1, the other lines have widths of 1km s-1. Towards L1448-mm, all lines except those of SiO and HCO, show two distinct velocity components centered at 4.7 and 5.2 km s-1. HCO is only observed in the 4.7 km s-1 cloud, and SiO in the 5.2 km s-1 component. The SiO abundance is 10E-11 in the 5.2 km s-1 clouds, one order of magnitude larger than in the 4.7 km s-1 component and in other dark clouds. The HCO abundance is 10E-11, similar to that predicted by the ion-molecule reactions models for the quiescent gas in dark clouds. The large change in the SiO/HCO abundance ratio (>150) from the 4.7 to the 5.2 km s-1 component, and the distribution and kinematics of the SiO emission towards L1448-mm suggest that the ambient SiO is associated with the molecular outflows. We propose that the narrow linewidths and the abundances of SiO in the ambient gas are produced by the interaction of the magnetic and/or radiative precursors of the shocks with the clumpy pre-shocked ambient gas.
机译:我们提出了在环境速度下朝向SiO v = 0 J = 2-1和J = 3-2线以及HCO 101-000 J = 3 / 2-1 / 2 F = 2-1线的检测。 L1448-mm和L1448-IRS3中的分子流出。这是在暗云中首次检测到HCO。我们还测量了H13CO +,H13CN,HN13C,CH3OH和N2H +的谱线。 HCO和SiO线的轮廓最窄,线宽为0.5 km s-1,其他线的宽度为1km s-1。朝向L1448-mm,除SiO和HCO的所有线外,其他两个线均显示出两个不同的速度分量,分别位于4.7 km和5.2 km s-1处。仅在4.7 km s-1云中观测到HCO,而在5.2 km s-1云中观测到SiO。 5.2 km s-1云中的SiO丰度为10E-11,比4.7 km s-1组分和其他暗云中的SiO丰度大一个数量级。 HCO丰度为10E-11,类似于通过离子-分子反应模型预测的乌云中静态气体的丰度。 SiO / HCO丰度比(> 150)从4.7 km s-1到5.2 km s-1发生了很大变化,并且SiO朝L1448-mm方向的发射分布和运动学研究表明,环境SiO与分子流出有关。我们提出,环境气体中较窄的线宽和SiO的丰度是通过冲击的磁性和/或辐射前体与块状预震环境气体的相互作用而产生的。

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