论文标题

从大型麦哲伦云的星际灰尘与普朗克揭示了两极分化的发射

Unveiling polarized emission from interstellar dust of the Large Magellanic Cloud with Planck

论文作者

Alina, D., Bernard, J. -Ph., Yuen, K. H., Lazarian, A., Hughes, A., Iskakova, M., Akimkhan, A., Mukanova, A.

论文摘要

星际灰尘发射的极化是粉尘特性和磁场结构的强大探针。然而,外部星系的研究受到前景灰尘贡献的阻碍。这项研究的目的是将极化信号与大型麦哲伦云(LMC)与银河系(MW)的偏振信号分开,以便使用Planck 353 GHz数据构建宽场,空间完整的尘埃极化图。为了估计前景极化方向,我们使用了HI光谱线数据中的速度梯度,并通过比较星光消光极化来评估输出的性能。我们使用先前从Planck数据得出的灰尘特性来估计前景强度,我们假设前景极化是均匀的,并且等于银河系周围的MW的平均值。前景去除后,LMC中天空磁场的几何形状倾向于遵循LMC中原子气的结构。沿着分子脊延伸到30多拉多斯恒星形成综合体的南部和东南部,沿着更漫射的南部臂延伸到小麦芽岩云,沿着分子山脊向南和东南延伸的分子脊而言,尤其是这种情况。西部的磁场和外臂之间也有一个对齐。 LMC中的中间极化分数略低于MW观察到的,而极化角度分散函数和极化分数之间的抗相关性略大。总体而言,极化分数分布与MW中观察到的分布相似。

Polarization of interstellar dust emission is a powerful probe of dust properties and magnetic field structure. Yet studies of external galaxies are hampered by foreground dust contribution. The aim of this study is to separate the polarised signal from the Large Magellanic Cloud (LMC) from that of the Milky Way (MW) in order to construct a wide-field, spatially complete map of dust polarization using the Planck 353 GHz data. To estimate the foreground polarization direction, we used velocity gradients in HI spectral line data and assessed the performance of the output by comparing to starlight extinction polarization. We estimate the foreground intensity using dust properties derived previously from the Planck data and we assume the foreground polarization to be uniform and equal to the average of the MW around the galaxy. After foreground removal, the geometry of the plane-of-the-sky magnetic field in the LMC tends to follow the structure of the atomic gas in the LMC. This is notably the case along the molecular ridges extending south and south-east of the 30 Doradus star-forming complex, and along more diffuse southern arm extending towards the Small Magellanic Cloud. There is also an alignment between the magnetic field and the outer arm in the western part. The median polarization fraction in the LMC is slightly lower than that observed for the MW while the anti-correlation between the polarization angle dispersion function and the polarization fraction is slightly larger. Overall, polarization fraction distribution is similar to that observed in the MW.

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