利用闵科夫斯基函数探测波动动力学诱导的偏振发射形态

Riju Dutta, Sharanya Sur, Aritra Basu
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摘要

极化结构的形态和特征尺度为了解磁离子等离子体中驱动湍流和维持磁场的机制提供了重要信息。我们的目标是建立闵科夫斯基函数作为波动动力学作用产生的极化同步辐射丝状形态的定量统计探针的有效性。利用等温、不可压缩和亚音速介质中不同驱动尺度($\ell_{\rm f}$)湍流的波动动力学模拟产生的合成观测结果,我们研究了不同形态测量之间的关系,以及它们与分数极化($p_\{rm f}$)之间的联系。我们发现,法拉第去极化在低频下产生的小尺度极化结构与与$ell_{\rm f}$相当的本征结构相比,具有更高的丝状性。在超过 $sim3\,{\rm GHz}$ 时,单位面积上连接的极化结构的数量($N_{\rm CC, peak}$)与发射区域的平均 $p_{rmf}$ ($\langle p_{\rm f} \rangle$)相关,即 $\langle p_{\rm f} \rangle \propto N_{\rm CC、peak}^{-1/4}$ ,前提是可探测发射区域的尺度大于 $\ell_{\rm f}$。这意味着$N_{rmCC,peak}$ 代表了投影在天空平面上的湍流单元的数量,可以通过关系式$ell_{\rm f} 直接用于推断$ell_{\rm f} $。\propto N_{{rm CC,peak}^{-1/2}$.对 $\ell_{\rm f}$ 的估计可以直接确定物理系统中的湍流驱动机制。虽然模拟的条件主要是星系团的团内介质,但定性的形态特征也适用于星系中的星际介质。
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Probing the morphology of polarized emission induced by fluctuation dynamo using Minkowski functionals
The morphology and the characteristic scale of polarized structures provide crucial insights into the mechanisms that drives turbulence and maintains magnetic fields in magneto-ionic plasma. We aim to establish the efficacy of Minkowski functionals as quantitative statistical probes of filamentary morphology of polarized synchrotron emission resulting from fluctuation dynamo action. Using synthetic observations generated from magnetohydrodynamic simulations of fluctuation dynamos with varying driving scales ($\ell_{\rm f}$) of turbulence in isothermal, incompressible, and subsonic media, we study the relation between different morphological measures, and their connection to fractional polarization ($p_{\rm f}$). We find that Faraday depolarization at low frequencies give rise to small-scale polarized structures that have higher filamentarity as compared to the intrinsic structures that are comparable to $\ell_{\rm f}$. Above $\sim3\,{\rm GHz}$, the number of connected polarized structures per unit area ($N_{\rm CC, peak}$) is related to the mean $p_{\rm f}$ ($\langle p_{\rm f} \rangle$) of the emitting region as $\langle p_{\rm f} \rangle \propto N_{\rm CC, peak}^{-1/4}$, provided the scale of the detectable emitting region is larger than $\ell_{\rm f}$. This implies that $N_{\rm CC,peak}$ represents the number of turbulent cells projected on the plane of the sky and can be directly used to infer $\ell_{\rm f}$ via the relation $\ell_{\rm f} \propto N_{\rm CC,peak}^{-1/2}$. An estimate on $\ell_{\rm f}$ thus directly allows for pinning down the turbulence driving mechanism in astrophysical systems. While the simulated conditions are mostly prevalent in the intracluster medium of galaxy clusters, the qualitative morphological features are also applicable in the context of interstellar medium in galaxies.
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