大质量恒星形成区的磁场(MagMaR):利用 ALMA 揭示 G333.46-0.16 中的沙漏磁场

Piyali Saha, Patricio Sanhueza, Marco Padovani, Josep M. Girart, Paulo C. Cortés, Kaho Morii, Junhao Liu, Á. Sánchez-Monge, Daniele Galli, Shantanu Basu, Patrick M. Koch, Maria T. Beltrán, Shanghuo Li, Henrik Beuther, Ian W. Stephens, Fumitaka Nakamura, Qizhou Zhang, Wenyu Jiao, M. Fernández-López, Jihye Hwang, Eun Jung Chung, Kate Pattle, Luis A. Zapata, Fengwei Xu, Fernando A. Olguin, Ji-hyun Kang, Janik Karoly, Chi-Yan Law, Jia-Wei Wang, Timea Csengeri, Xing Lu, Yu Cheng, Jongsoo Kim, Spandan Choudhury, Huei-Ru Vivien Chen, Charles L. H. Hull
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引用次数: 0

摘要

人们对磁场对高质恒星形成的贡献知之甚少。我们报告了高角分辨率(∼0.″3,870 au)的磁场投影在天空平面(BPOS)上的地图,该地图是高质恒星形成区 G333.46-0.16 (G333)的一部分,由阿塔卡马大型毫米波/亚毫米波阵列在 1.2 毫米处获得,是大质量恒星形成区磁场测量的一部分。在该区域发现的 BPOS 形状与典型的 "沙漏 "一致,在垂直方向上有一个嵌入的扁平包膜,这表明存在一个重要的动态磁场。这个区域分裂成两颗原恒星,它们似乎在引力作用下结合成一个稳定的双星系统,相距 ∼ 1740 au。有趣的是,通过分析 H13CO+ (J = 3-2) 线发射,我们发现在连续面的范围内没有速度梯度,这与强场是一致的。我们对 BPOS 进行了建模,得到了 1.43 的微弱超临界质量流量比,这表明最初的环境具有很强的磁性。根据 Davis-Chandrasekhar-Fermi 方法,G333 的磁场强度估计为 5.7 mG。G333中心区域没有强烈的旋转和外流,这表明它具有很强的磁制动能力,与高磁化环境相一致。我们的研究表明,尽管磁能是一个强大的调节器,但它并不能阻止碎裂过程,正如中心区域两颗原恒星的形成所揭示的那样。
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Magnetic Fields in Massive Star-forming Regions (MagMaR): Unveiling an Hourglass Magnetic Field in G333.46–0.16 Using ALMA
The contribution of the magnetic field to the formation of high-mass stars is poorly understood. We report the high angular resolution (∼0.″3, 870 au) map of the magnetic field projected on the plane of the sky (B POS) toward the high-mass star-forming region G333.46−0.16 (G333), obtained with the Atacama Large Millimeter/submillimeter Array at 1.2 mm as part of the Magnetic fields in Massive star-forming Regions survey. The B POS morphology found in this region is consistent with a canonical “hourglass” with an embedded flattened envelope in a perpendicular direction, which suggests a dynamically important field. This region is fragmented into two protostars that appear to be gravitationally bound in a stable binary system with a separation of ∼1740 au. Interestingly, by analyzing H13CO+ (J = 3–2) line emission, we find no velocity gradient over the extent of the continuum, which is consistent with a strong field. We model the B POS, obtaining a marginally supercritical mass-to-flux ratio of 1.43, suggesting an initially strongly magnetized environment. Based on the Davis–Chandrasekhar–Fermi method, the magnetic field strength toward G333 is estimated to be 5.7 mG. The absence of strong rotation and outflows toward the central region of G333 suggests strong magnetic braking, consistent with a highly magnetized environment. Our study shows that despite being a strong regulator, the magnetic energy fails to prevent the process of fragmentation, as revealed by the formation of the two protostars in the central region.
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