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首页> 外文期刊>The Astrophysical journal >Magnetic Fields in Star-forming Molecular Clouds. V. Submillimeter Polarization of the Barnard 1 Dark Cloud
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Magnetic Fields in Star-forming Molecular Clouds. V. Submillimeter Polarization of the Barnard 1 Dark Cloud

机译:恒星形成分子云中的磁场。 V.巴纳德1暗云的亚毫米波极化

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We present 850 μm polarimetry from the James Clerk Maxwell Telescope toward several dense cores within the dark cloud Barnard 1 in Perseus. Significant polarized emission is detected from across the mapped area and is not confined to the locations of bright cores. This indicates the presence of aligned grains and hence a component of the magnetic field in the plane of the sky. Polarization vectors detected away from bright cores are strongly aligned at a position angle of ~90° (east of north), while vectors associated with bright cores show alignments of varying orientations. There is no direct correlation between the polarization angles measured in earlier optical polarimetry toward Perseus and the polarized submillimeter thermal emission. Depolarization toward high intensities is exhibited but toward the brightest core reaches a threshold beyond which no further decrease in polarization percentage is measured. The polarized emission data from the interior envelope are compared with previously published OH Zeeman data to estimate the total field strength and orientation under the assumption of a uniform and nonuniform field component in the region. These results are rough estimates only as a result of the single independent detection of Zeeman splitting toward Barnard 1. The uniform field component is thus calculated to be 0 = 31 μG [±(0.52 - 0.01) - 0.86] in the case in which we have assumed the ratio of the dispersion of the line-of-sight field to the field strength to be 0.2.
机译:我们提出了从James Clerk Maxwell望远镜向珀尔修斯(Perseus)的黑云Barnard 1内的几个致密核心进行850μm偏振的方法。从整个地图区域检测到明显的极化发射,并且不限于亮芯的位置。这表明存在排列的晶粒,因此表明在天空平面中存在磁场分量。远离亮芯检测到的极化矢量在〜90°(北偏东)的位置角处强烈对准,而与亮芯相关的矢量显示出不同方向的对准。在较早的朝向珀尔修斯的光学偏振法中测量的偏振角与偏振的亚毫米热发射之间没有直接关系。表现出朝向高强度的去极化,但是朝向最亮的核心达到一个阈值,超过该阈值则无法测量极化百分比的进一步降低。将内部包络的极化发射数据与先前发布的OH Zeeman数据进行比较,以在该区域均匀且不均匀的场分量的假设下估算总场强和方向。这些结果仅是对Zeeman向Barnard 1分裂的一次独立检测的结果的粗略估计。因此,在以下情况下,均匀场分量计算为0 = 31μG[±(0.52-0.01)-0.86]。假定视场色散与场强之比为0.2。

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