重新审视大质量恒星形成复合体 RCW 122:新的毫米波和亚毫米波研究

N. Duronea, L. Bronfman, M. Ortega, L. Suad, G. Baume, E. Mendoza, M. Carvajal, S. Cichowolski, E. M. Arnal, R. Finger, M. Merello, R. Gamen
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引用次数: 0

摘要

在本文中,我们对巨型恒星形成复合体 RCW\,122 进行了一项新的多频研究。我们使用了 ASTE 10 m 和 APEX 12 m 望远镜获得的分子数据,以及从现有数据库中获得的从 3.6 到 870 波段的红外观测数据。我们还纳入了一系列公共数据集,包括 3 GHz 的射电连续波、窄带 Halpha 图像和深度 JHK 测光。我们的分析主要集中在编录的ATLASGAL源上,展示了从红外暗云(IRDC)/高质原恒星天体(HMPO)到超小型HII区(UCHII)等演化阶段的光谱,这是从对公共数据集的初步检查中推断出来的。根据ASTE HCO$^+$(4--3)和CO(3--2)数据,我们确定了五个分子团块,分别命名为A、B、C、D和E,作为ATLASGAL源的分子对应物。这些分子团块的径向速度从sim --15 到 --10,证实了它们与RCW,122的联系。此外,我们还报告说在APEX光谱的228.538 GHz到232.538 GHz和218.3到222.3 GHz频率范围内探测到了来自11种不同分子的20次跃迁,揭示了星团中复杂多样的化学成分。利用 APEX 望远镜观测到的 CO(2--1) 和 C18O(2--1) 数据,我们估算出了 LTE 的总分子质量,范围从 200M_ odot $(星团 A)到 4400M_ odot $(星团 B)。我们的中远红外(MIR-FIR)通量密度分析得出尘埃的最低温度为 23.7 K(星团 A),最高温度为 33.9 K(星团 B),这表明星团之间存在不同程度的内部加热。测光度从 1.7times 10$^3$ L$_ odot $(星团 A)到 2.4times 10$^5$ L$_ odot $(星团 B)不等,而总质量(尘埃+气体)从 350 $M_ odot $(星团 A)到 3800 $M_ odot $(星团 B)不等。我们对分子线丰富度、$L/M$比值、CH$_3$CCH和尘埃温度的分析表明,A/Erightarrow Crightarrow D/B的演化序列与ATLASGAL源的初步推断一致。在这种情况下,星团 A 和 E 显示出坍缩的早期阶段,星团 A 很可能处于早期 HMPO 阶段,这一点可以通过识别候选分子外流得到支持。星团 E 似乎处于 IRDC 和 HMPO 之间的中间阶段。星团 D 和 B 显示出处于 UCHII 阶段的迹象,其中星团 B 可能更晚些。团块 C 可能处于 HMPO 和 HMC 之间的中间阶段。我们的研究结果表明,星团DBS\,119的多个恒星和原恒星成员正在对星团B进行电离和加热。同时,星团的其他成员也可能负责电离 RCW\,122 的其他区域,这些区域已经演化成发育完全的 HII 区域,超过了分子解离阶段。
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Revisiting the massive star-forming complex RCW 122: New millimeter and submillimeter study
In this paper, we present a new multifrequency study of the giant star-forming complex RCW\,122. We used molecular data obtained with the ASTE 10 m and the APEX 12 m telescopes, along with infrared observations spanning from 3.6 to 870 obtained from available databases. We also incorporated a range of public datasets, including the radio continuum at 3 GHz, narrowband Halpha images, and deep JHK photometry. Our analysis focuses mostly on cataloged ATLASGAL sources, showcasing a spectrum of evolutionary stages from infrared dark cloud (IRDC)/high-mass protostellar object (HMPO) to ultra-compact HII region (UCHII), as inferred from preliminary inspections of the public dataset. Based on ASTE HCO$^+$(4--3) and CO(3--2) data, we identified five molecular clumps, designated A, B, C, D, and E, as molecular counterparts of the ATLASGAL sources. These clumps have radial velocities ranging from sim --15 to --10 confirming their association with RCW\,122. In addition, we report the detection of 20 transitions from 11 distinct molecules in the APEX spectra in the frequency ranges from 228.538 GHz to 232.538 GHz and 218.3 to 222.3 GHz, unveiling a diverse chemical complexity among the clumps. Utilizing CO(2--1) and C18O(2--1) data taken from the observations with the APEX telescope we estimated the total LTE molecular mass, ranging from 200 $M_ odot $ (clump A) to 4400 $M_ odot $ (clump B). Our mid- to far-infrared (MIR-FIR) flux density analysis yielded minimum dust temperatures of 23.7 K (clump A) to maximum temperatures of 33.9 K (clump B), indicating varying degrees of internal heating among the clumps. The bolometric luminosities span 1.7times 10$^3$ L$_ odot $ (clump A) to 2.4times 10$^5$ L$_ odot $ (clump B), while the total (dust+gas) mass ranges from 350 $M_ odot $ (clump A) to 3800 $M_ odot $ (clump B). Our analysis of the molecular line richness, $L/M$ ratios, and CH$_3$CCH and dust temperatures reveals an evolutionary sequence of A/Erightarrow Crightarrow D/B, consistent with preliminary inferences of the ATLASGAL sources. In this context, clumps A and E exhibit early stages of collapse, with clump A likely in an early HMPO phase, which is supported by identifying a candidate molecular outflow. Clump E appears to be in an intermediate stage between IRDC and HMPO. Clumps D and B show evidence of being in the UCHII phase, with clump B likely more advanced. Clump C likely represents an intermediate stage between HMPO and HMC. Our findings suggest clump B is undergoing ionization and heating by multiple stellar and protostellar members of the stellar cluster DBS\,119. Meanwhile, other cluster members may be responsible for ionizing other regions of RCW\,122 that have evolved into fully developed HII regions, beyond the molecular dissociation stage.
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