首页> 外文期刊>Astronomy and astrophysics >The magnetic precursor of L1448-mm: excitation differences between ion and neutral fluids
【24h】

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

机译:L1448-mm的磁性前驱体:离子流体与中性流体之间的激发差异

获取原文
           

摘要

Context. Shock modelling predicts an electrondensity enhancement within the magnetic precursor of C-shocks. Previousobservations of SiO, H13CO+,HN13C and H13CN towardthe young L1448-mm outflow showed an over-excitation of the ion fluidthat was attributed to an electron density enhancement in theprecursor. Aims. We re-visit this interpretation and test if itstill holds when we consider different source morphologies and kinetictemperatures for the observed molecules. To do this, we use updatedcollisional coefficients of HN13C and SiO withelectrons in our excitation model. We also aim to give some insight onthe spatial extent of the electron density enhancement around L1448-mm.Methods. We estimate the opacities of H13CO+and HN13C by observing thelinesof rarer isotopologues. To model the excitation of the molecules, weuse the large velocity gradient (LVG) approximation with updatedcollisional coefficients to i) re-analyse the observations toward thepositions where the over-excitation of H13CO+has previously been observed [i.e. toward L1448-mm at offsets(0,0) and (0, -10)]; and ii) to investigate if the electrondensity enhancement is still required for the cases of extended andcompact emission, and for kinetic temperatures of up to 400K.We also report several lines of SiO, HN13C and H13CO+toward new positions around this outflow, to investigate the spatialextent of the over-excitation of the ions in L1448-mm. Results. From the isotopologue observations, we findthat the emission of H13CO+and HN13C from the precursor is optically thinif this emission is extended. Using the new collisional coefficients,an electron density enhancement is still needed to explain theexcitation of H13CO+ forextended emission and for gas temperatures of 400K toward L1448-mm (0, -10), andpossibly also toward L1448-mm (0,0). For compact emission thedata cannot be fitted. We do not find any evidence for theover-excitation of the ion fluid toward the newly observed positionsaround L1448-mm. Conclusions. 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 theprecursor component, if this emission is spatially extended. This isalso true for the case of high gas temperatures (400K)toward the (0, -10) offset. The electron density enhancement seems tobe restricted to the southern, redshifted lobe of the L1448-mm outflow.Interferometric images of the line emission of these molecules areneeded to confirm the spatial extent of the over-excitation of the ionsand thus, of the electron density enhancement in the magnetic precursorof L1448-mm. Key words: ISM: individual objects: L1448- ISM: clouds - ISM: jets and outflows - ISM: molecules - shock waves
机译:上下文。冲击模型预测C冲击的磁性前驱体内电子密度会提高。先前对年轻的L1448-mm流出的SiO,H13CO +,HN13C和H13CN的观察表明,离子流体过度激发,这归因于前体中电子密度的提高。目的当我们考虑所观察到的分子的不同来源形态和动力学温度时,我们将重新解释该解释并测试它是否仍然成立。为此,我们在激发模型中使用了HN13C和SiO与电子的更新碰撞系数。我们还旨在对L1448-mm附近电子密度增强的空间范围提供一些见识。我们通过观察稀有同位素分子的谱线估计H13CO +和HN13C的不透明性。为了对分子的激发进行建模,我们使用具有更新的碰撞系数的大速度梯度(LVG)近似来i)对先前已观察到H13CO +过度激发的位置重新进行观察[[e.e.朝L1448-mm偏移(0,0)和(0,-10)]]; ii)研究在扩展和紧凑发射的情况下以及高达400K的动力学温度下是否仍需要提高电子密度。我们还报告了SiO,HN13C和H13CO +在此流出附近向新位置移动的几条线,以进行调查L1448-mm中离子过度激发的空间范围。结果。从同位素同位素观察,我们发现,如果延长了前体的H13CO +和HN13C的发射,光学上就很薄。使用新的碰撞系数,仍然需要电子密度的增强来解释H13CO +的激发,用于扩展发射以及气体温度为400K时朝L1448-mm(0,-10),还可能朝L1448-mm(0,0)。为了紧凑发射,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附近新观察到的位置过度激发。结论。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。对于较高的气体温度(400K)接近(0,-10)偏移的情况也是如此。电子密度的增强似乎仅限于L1448-mm流出的南部红移波瓣。需要这些分子的线发射的干涉图来确认离子过度激发的空间范围,从而确定电子密度的增强在L1448-mm的磁性前体中。关键词:ISM:单个物体:L1448- ISM:云-ISM:喷流和流出-ISM:分子-冲击波

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号