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The Origin of [C ii] 157 μm Emission in a Five-component Interstellar Medium: The Case of NGC 3184 and NGC 628

机译:五组分星际介质中[C ii] 157μm辐射的起源:以NGC 3184和NGC 628为例

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With its relatively low ionization potential, C+ can be found throughout the interstellar medium (ISM) and provides one of the main cooling channels of the ISM via the [C ii] 157 μm emission. While the strength of the [C ii] line correlates with the star formation rate, the contributions of the various gas phases to the [C ii] emission on galactic scales are not well established. In this study we establish an empirical multi-component model of the ISM, including dense H ii regions, dense photon dissociation regions (PDRs), the warm ionized medium (WIM), low density and ?surfaces of molecular clouds (SfMCs), and the cold neutral medium (CNM). We test our model on ten luminous regions within the two nearby galaxies NGC 3184 and NGC 628?on angular scales of 500–600 pc. Both galaxies are part of the Herschel?key program?KINGFISH,?and are complemented by a large set of ancillary ground- and space-based data. The five modeled phases together reproduce the observed [C ii] emission quite well, overpredicting the total flux slightly (about 45%) averaged over all regions. We find that dense PDRs are the dominating component, contributing 68% of the [C ii] flux on average, followed by the WIM and the SfMCs, with mean contributions of about half of the contribution from dense PDRs, each. CNM and dense H ii regions are only minor contributors with less than 5% each. These estimates are averaged over the selected regions, but the relative contributions of the various phases to the [C ii] flux vary significantly between these regions.
机译:由于C +的电离势较低,因此可以在整个星际介质(ISM)中找到C +,并通过[C ii] 157μm辐射提供ISM的主要冷却通道之一。尽管[C ii]线的强度与恒星形成率相关,但在银河尺度上,各种气相对[C ii]发射的贡献还没有很好地确定。在这项研究中,我们建立了一个ISM的经验多成分模型,包括密集的H ii区,密集的光子解离区(PDR),温暖的电离介质(WIM),低密度和分子云的表面(SfMC),以及冷中性培养基(CNM)。我们在两个相邻星系NGC 3184和NGC 628?的十个发光区域上以500–600 pc的角尺度测试了我们的模型。这两个星系都是Herschel关键程序“金鱼”的一部分,并辅以大量的辅助地面和空基数据。五个建模阶段很好地重现了观察到的[C ii]发射,对所有区域的平均总通量略有过高(大约45%)的预测。我们发现密集的PDR是主要的组成部分,平均贡献了[C ii]通量的68%,其次是WIM和SfMC,平均贡献分别约为密集的PDR的一半。 CNM和密集的H ii地区仅是较小的贡献者,每个贡献者少于5%。这些估计值是在所选区域内平均的,但是各个区域在[C ii]通量方面的相对贡献在这些区域之间差异很大。

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