Treviño-Morales S P, Fuente A, Sánchez-Monge Á, Pilleri P, Goicoechea J R, Ossenkopf-Okada V, Roueff E, Rizzo J R, Gerin M, Berné O, Cernicharo J, Gónzalez-García M, Kramer C, García-Burillo S, Pety J
Instituto de Ciencia de Materiales de Madrid, Sor Juana Inés de la Cruz 3, E-28049 Cantoblanco, Madrid, (Spain); Observatorio Astronómico Nacional, Apdo. 112, E-28803 Alcalá de Henares Madrid, (Spain).
Observatorio Astronómico Nacional, Apdo. 112, E-28803 Alcalá de Henares Madrid, (Spain).
Astron Astrophys. 2016 Sep 15;593. doi: 10.1051/0004-6361/201628899.
The CO reactive ion is thought to be a tracer of the boundary between a HII region and the hot molecular gas. In this study, we present the spatial distribution of the CO rotational emission toward the Mon R2 star-forming region. The CO emission presents a clumpy ring-like morphology, arising from a narrow dense layer around the HII region. We compare the CO distribution with other species present in photon-dominated regions (PDR), such as [CII] 158 m, H S(3) rotational line at 9.3 m, polycyclic aromatic hydrocarbons (PAHs) and HCO. We find that the CO emission is spatially coincident with the PAHs and [CII] emission. This confirms that the CO emission arises from a narrow dense layer of the HI/H interface. We have determined the CO fractional abundance, relative to C toward three positions. The abundances range from 0.1 to 1.9 ×10 and are in good agreement with previous chemical model, which predicts that the production of CO in PDRs only occurs in dense regions with high UV fields. The CO linewidth is larger than those found in molecular gas tracers, and their central velocity are blue-shifted with respect to the molecular gas velocity. We interpret this as a hint that the CO is probing photo-evaporating clump surfaces.
CO 反应离子被认为是 HII 区与热分子气体之间边界的示踪剂。在本研究中,我们展示了朝向麒麟座 R2 恒星形成区的 CO 转动发射的空间分布。CO 发射呈现出团块状的环状形态,源于 HII 区周围的一个狭窄致密层。我们将 CO 的分布与光子主导区(PDR)中存在的其他物种进行了比较,例如[CII]158 微米、9.3 微米处的 H S(3)转动线、多环芳烃(PAH)和 HCO。我们发现 CO 发射在空间上与 PAH 和[CII]发射重合。这证实了 CO 发射源于 HI/H 界面的一个狭窄致密层。我们已经确定了相对于 C 在三个位置的 CO 分数丰度。丰度范围为 0.1 至 1.9×10,与先前的化学模型高度一致,该模型预测 PDR 中 CO 的产生仅发生在具有高紫外场的致密区域。CO 的线宽大于在分子气体示踪剂中发现的线宽,并且它们的中心速度相对于分子气体速度发生蓝移。我们将此解释为一个迹象,表明 CO 正在探测光蒸发团块表面。