创造之柱中的磁场

Adwitiya Sarkar, Leslie W. Looney, Marc W. Pound, Zhi-Yun Li, Ian W. Stephens, Manuel Fernández-López, Simon Coudé, Zhe-Yu Daniel Lin, Haifeng Yang and Reid Faistl
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摘要

由于尘埃颗粒与磁场对齐,冷分子云的远红外辐射的尘埃偏振观测经常被用来追踪磁场,从而可以探测磁场对恒星形成过程的影响。我们利用平流层红外天文观测台/高分辨率机载宽带相机,从89和154 μm连续体的尘埃偏振数据中推断出了M16发射星云中创造之柱区域的磁场图。我们使用戴维斯-钱德拉塞卡-费米方法推导出磁场强度估计。我们将极化和磁场强度与整个地区的柱密度和尘埃连续体强度进行比较,以建立该地区恒星形成活动与磁场之间关系的连贯图像。得到的投影磁场强度在~ 50-130 μG范围内,这是类似n(H2)云的典型特征,即分子氢体积密度在104-105 cm−3量级。我们得出的结论是,当磁场太弱而无法阻止引力引起的径向坍缩,但又足够强以对抗OB恒星的辐射压力时,恒星形成发生在指尖,而在指底,磁场阻碍质量吸积,从而阻碍恒星形成。我们还支持一个初始弱场模型(<50 μG),随后通过重新排列和压缩而增强,从而形成一个动态重要的磁场。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Magnetic Fields in the Pillars of Creation
Due to dust grain alignment with magnetic fields, dust polarization observations of far-infrared emission from cold molecular clouds are often used to trace magnetic fields, allowing a probe of the effects of magnetic fields on the star formation process. We present inferred magnetic field maps of the Pillars of Creation region within the larger M16 emission nebula, derived from dust polarization data in the 89 and 154 μm continuum using the Stratospheric Observatory For Infrared Astronomy/High-resolution Airborne Wideband Camera. We derive magnetic field strength estimates using the Davis–Chandrasekhar–Fermi method. We compare the polarization and magnetic field strengths to column densities and dust continuum intensities across the region to build a coherent picture of the relationship between star-forming activity and magnetic fields in the region. The projected magnetic field strengths derived are in the range of ∼50–130 μG, which is typical for clouds of similar n(H2), i.e., molecular hydrogen volume density on the order of 104–105 cm−3. We conclude that star formation occurs in the finger tips when the magnetic fields are too weak to prevent radial collapse due to gravity but strong enough to oppose OB stellar radiation pressure, while in the base of the fingers the magnetic fields hinder mass accretion and consequently star formation. We also support an initial weak-field model (<50 μG) with subsequent strengthening through realignment and compression, resulting in a dynamically important magnetic field.
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