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The magnetic precursor of L1448-mm: Excitation differences between ion and neutral fluids

机译:L1448-mm的磁性前体:离子之间的激发差异   和中性液体

摘要

Shock modelling predicts an electron density enhancement within the magneticprecursor of C-shocks. Previous observations of SiO, H13CO+, HN13C and H13CNtoward the young L1448-mm outflow showed an over-excitation of the ion fluidthat was attributed to an electron density enhancement in the precursor. Were-visit this interpretation and test if it still holds when we considerdifferent source morphologies and kinetic temperatures for the observedmolecules, and also give some insight on the spatial extent of the electrondensity enhancement around L1448-mm. We estimate the opacities of H13CO+ and HN13C by observing the J=3\to2 linesof rarer isotopologues to confirm that the emission is optically thin. To modelthe excitation of the molecules, we use the large velocity gradient (LVG)approximation with updated collisional coefficients to i) re- analyse theobservations toward the positions where the over-excitation of H13CO+ haspreviously been observed [i.e. toward L1448- mm at offsets (0,0) and (0,-10)],and ii) to investigate if the electron density enhancement is still requiredfor the cases of extended and compact emission, and for kinetic temperatures ofup to 400 K. We also report several lines of SiO, HN13C and H13CO+ toward newpositions around this outflow, to investigate the spatial extent of theover-excitation of the ions in L1448-mm. From the isotopologue observations, wefind that the emission of H13CO+ and HN13C from the precursor is optically thinif this emission is extended. Using the new collisional coefficients, anelectron density enhancement is still needed to explain the excitation ofH13CO+ for extended emission and for gas temperatures of\le 400 K towardL1448-mm (0,-10), and possibly also toward L1448-mm (0,0). For compact emissionthe data cannot be fitted. We do not find any evidence for the over-excitationof the ion fluid toward the newly observed positions around L1448-mm. The observed line emission of SiO, H13CO+ and HN13C toward L1448-mm (0,0) and(0,-10) is consistent with an electron density enhancement in the precursorcomponent, if this emission is spatially extended. This is also true for thecase of high gas temperatures (\le400 K) toward the (0,-10) offset. Theelectron density enhancement seems to be restricted to the southern, redshiftedlobe of the L1448-mm outflow. Interferometric images of the line emission ofthese molecules are needed to confirm the spatial extent of the over-excitationof the ions and thus, of the electron density enhancement in the magneticprecursor of L1448-mm.
机译:冲击模型预测C冲击的磁前驱体内电子密度会提高。 SiO,H13CO +,HN13C和H13CN往年轻的L1448-mm流出处的先前观察结果表明,离子流体过度激发,这归因于前体中电子密度的提高。考察了这种解释并测试了当我们考虑所观察到的分子的不同源形态和动力学温度时是否仍然成立,并且还对L1448-mm附近电子密度增强的空间范围提供了一些见识。我们通过观察稀有同位素分子的J = 3 \ to2谱线来估计H13CO +和HN13C的不透明性,以确认发射光很薄。为了模拟分子的激发,我们使用具有更新的碰撞系数的大速度梯度(LVG)逼近来i)重新分析观察到以前观察到H13CO +过度激发的位置[即。在偏移(0,0和(0,-10)处向L1448-mm方向移动),以及ii)研究在扩展和紧凑发射的情况下以及高达400 K的动力学温度下是否仍需要提高电子密度。我们还报告了几条SiO,HN13C和H13CO +线朝着此流出附近的新位置移动,以研究L1448-mm中离子过度激发的空间范围。从同位素共聚体观察,我们发现,如果延长了前体的H13CO +和HN13C的发射,则该发射在光学上较薄。使用新的碰撞系数,仍然需要电子密度增强来解释H13CO +的激发,以进行扩展发射以及气体温度朝着L1448-mm(0,-10)和可能达到L1448-mm(0,0)达到\ le 400 K )。对于紧凑型发射器,无法安装数据。我们没有发现任何证据表明离子流体向L1448-mm附近的新观察位置过度激发。如果在空间上扩展,观察到的SiO,H13CO +和HN13C向L1448-mm(0,0)和(0,-10)的线发射与前体组分中的电子密度增强相一致。对于向(0,-10)偏移的较高气体温度(\ le400 K)的情况也是如此。电子密度的增强似乎仅限于L1448-mm流出的南部红移波瓣。这些分子的线发射的干涉图图像需要确认离子过度激发的空间范围,从而确认L1448-mm磁性前体中电子密度的增强。

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