用宽波段极坐标测量法分解 NGC 6946 中的磁场

A. L. Williams, G. Heald, E. Wilcots, E. Zweibel
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摘要

我们利用韦斯特伯克合成射电望远镜(Westerbork Synthesis Radio Telescope,WSRT)对附近的螺旋星系NGC 6946进行了λ13厘米偏振观测,以研究近侧光环磁场。尽管λ13 厘米波长的二维形态与在更长(λ18-22 厘米)或更短(λ3 和 λ6 厘米)波长上观测到的二维形态相似,但要解释该星系西南象限的极化差距,还需要更完整的频率覆盖。我们根据WSRT、Karl G. Jansky超大阵列和Effelsberg望远镜的观测结果,将湍流磁场和相干视线磁场模型与λ3、λ6、λ13、λ18和λ22厘米处的线性偏振发射分数度进行了拟合。结果表明这是一种多层湍流磁电离介质,与目前对边缘星系的观测结果一致。我们对同步辐射薄盘和厚盘(尺度高度分别为 300 pc 和 1.4 kpc)以及热厚盘和晕(尺度高度分别为 1 kpc 和 5 kpc)的物理特性进行了约束。我们首选的模型显示,在中面 1 kpc 范围内有一个团块状的高湍流介质,以及一个法拉第去极化程度较低的弥漫平面外层。在光环中,我们估计规则磁场强度为 0.4-2.2 μG,湍流和 ∼6 μG 的总磁场强度导致了 σ RM = 4-48 rad m-2 的法拉第色散。这项工作是现代射电望远镜的先进功能如何为宇宙磁性研究开辟新领域的一个例子。
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Disentangling Magnetic Fields in NGC 6946 with Wide-band Polarimetry
We present λ13 cm polarization observations of the nearby spiral galaxy NGC 6946 with the Westerbork Synthesis Radio Telescope (WSRT) to examine the nearside halo magnetic fields. Despite λ13 cm exhibiting similar two-dimensional morphology as observed at longer (λ18–22 cm) or shorter (λ3 and λ6 cm) wavelengths, more complete frequency coverage will be required to explain the gap in polarization in the southwest quadrant of the galaxy. We fit models of the turbulent and coherent line-of-sight magnetic fields to the fractional degree of linearly polarized emission at λ3, λ6, λ13, λ18, and λ22 cm from observations taken with the WSRT, Karl G. Jansky Very Large Array, and Effelsberg telescopes. The results favor a multilayer turbulent magneto-ionized medium consistent with current observations of edge-on galaxies. We constrain the physical properties of the synchrotron-emitting thin and thick disks (scale heights of 300 pc and 1.4 kpc, respectively) along with the thermal thick disk and halo (scale heights of 1 and 5 kpc, respectively). Our preferred model indicates a clumpy and highly turbulent medium within 1 kpc of the midplane, and a diffuse extraplanar layer with a substantially lower degree of Faraday depolarization. In the halo, we estimate a regular magnetic field strength of 0.4–2.2 μG and that turbulence and a total magnetic field strength of ∼6 μG result in a Faraday dispersion of σ RM = 4–48 rad m−2. This work is an example of how the advanced capabilities of modern radio telescopes are opening a new frontier for the study of cosmic magnetism.
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