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猎户座B分子云中L1630的[Cii]发射。

[Cii] emission from L1630 in the Orion B molecular cloud.

作者信息

Pabst C H M, Goicoechea J R, Teyssier D, Berné O, Ochsendorf B B, Wolfire M G, Higgins R D, Riquelme D, Risacher C, Pety J, Le Petit F, Roueff E, Bron E, Tielens A G G M

机构信息

Leiden Observatory, Leiden University, P.O. Box 9513, 2300 RA Leiden, Netherlands.

ICMM-CSIC, Calle Sor Juana Ines de la Cruz 3, 28049 Cantoblanco, Madrid, Spain.

出版信息

Astron Astrophys. 2017 Oct;606. doi: 10.1051/0004-6361/201730881. Epub 2017 Oct 3.

Abstract

CONTEXT

L1630 in the Orion B molecular cloud, which includes the iconic Horsehead Nebula, illuminated by the star system Ori, is an example of a photodissociation region (PDR). In PDRs, stellar radiation impinges on the surface of dense material, often a molecular cloud, thereby inducing a complex network of chemical reactions and physical processes.

AIMS

Observations toward L1630 allow us to study the interplay between stellar radiation and a molecular cloud under relatively benign conditions, that is, intermediate densities and an intermediate UV radiation field. Contrary to the well-studied Orion Molecular Cloud 1 (OMC1), which hosts much harsher conditions, L1630 has little star formation. Our goal is to relate the [Cii] fine-structure line emission to the physical conditions predominant in L1630 and compare it to studies of OMC1.

METHODS

The [Cii] 158 m line emission of L1630 around the Horsehead Nebula, an area of 12' × 17', was observed using the upgraded German Receiver for Astronomy at Terahertz Frequencies (upGREAT) onboard the Stratospheric Observatory for Infrared Astronomy (SOFIA).

RESULTS

Of the [Cii] emission from the mapped area 95%, 13 , originates from the molecular cloud; the adjacent Hii region contributes only 5%, that is, 1 . From comparison with other data (CO(1-0)-line emission, far-infrared (FIR) continuum studies, emission from polycyclic aromatic hydrocarbons (PAHs)), we infer a gas density of the molecular cloud of ∼ 3 · 10 cm, with surface layers, including the Horsehead Nebula, having a density of up to ∼ 4 · 10 cm. The temperature of the surface gas is ∼ 100 K. The average [Cii] cooling efficiency within the molecular cloud is 1.3 · 10. The fraction of the mass of the molecular cloud within the studied area that is traced by [Cii] is only 8%. Our PDR models are able to reproduce the FIR-[Cii] correlations and also the CO(1-0)-[Cii] correlations. Finally, we compare our results on the heating efficiency of the gas with theoretical studies of photoelectric heating by PAHs, clusters of PAHs, and very small grains, and find the heating efficiency to be lower than theoretically predicted, a continuation of the trend set by other observations.

CONCLUSIONS

In L1630 only a small fraction of the gas mass is traced by [Cii]. Most of the [Cii] emission in the mapped area stems from PDR surfaces. The layered edge-on structure of the molecular cloud and limitations in spatial resolution put constraints on our ability to relate different tracers to each other and to the physical conditions. From our study, we conclude that the relation between [Cii] emission and physical conditions is likely to be more complicated than often assumed. The theoretical heating efficiency is higher than the one we calculate from the observed [Cii] emission in the L1630 molecular cloud.

摘要

背景

猎户座B分子云中的L1630,其中包括标志性的马头星云,由参宿星系统照亮,是一个光解离区域(PDR)的例子。在PDR中,恒星辐射撞击致密物质表面,通常是分子云,从而引发复杂的化学反应和物理过程网络。

目的

对L1630的观测使我们能够在相对温和的条件下研究恒星辐射与分子云之间的相互作用,即中等密度和中等紫外线辐射场。与研究充分的猎户座分子云1(OMC1)不同,后者的条件要恶劣得多,L1630几乎没有恒星形成。我们的目标是将[CII]精细结构线发射与L1630中占主导地位的物理条件联系起来,并将其与OMC1的研究进行比较。

方法

使用平流层红外天文台(SOFIA)上升级后的太赫兹频率德国天文学接收器(upGREAT)观测了马头星云周围12'×17'区域的L1630的[CII]158μm线发射。

结果

在测绘区域的[CII]发射中,95%(13 )来自分子云;相邻的HII区域仅贡献5%,即1 。通过与其他数据(CO(1-0)线发射、远红外(FIR)连续谱研究、多环芳烃(PAH)发射)的比较,我们推断分子云的气体密度约为3·10 cm,包括马头星云在内的表层密度高达约4·10 cm。表面气体温度约为100K。分子云内的平均[CII]冷却效率为1.3·10。在研究区域内由[CII]追踪到的分子云质量分数仅为8%。我们的PDR模型能够再现FIR-[CII]相关性以及CO(1-0)-[CII]相关性。最后,我们将气体加热效率的结果与PAH、PAH团簇和非常小的颗粒的光电加热理论研究进行比较,发现加热效率低于理论预测,这是其他观测所设定趋势的延续。

结论

在L1630中,只有一小部分气体质量由[CII]追踪到。测绘区域内的大部分[CII]发射来自PDR表面。分子云的分层边缘结构和空间分辨率的限制对我们将不同示踪剂相互关联以及与物理条件相关联的能力施加了限制。从我们的研究中,我们得出结论,[CII]发射与物理条件之间的关系可能比通常假设的更为复杂。理论加热效率高于我们根据L1630分子云中观测到的[CII]发射计算得出的效率。

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