论文标题
银河小规模的迪纳摩的Batchelor,Saffman和Kazantsev Spectra
Batchelor, Saffman, and Kazantsev spectra in galactic small-scale dynamos
论文作者
论文摘要
据信,星系簇中的磁场以及在星际介质中的磁场是由小型发电机产生的。从理论上讲,在其运动阶段,它的特征是kazantsev频谱,该光谱在电阻尺度上达到峰值。它仅比随机和因果连接的磁场所期望的Saffman频谱稍浅。因果关系断开的田地具有更陡峭的批量光谱。在这里,我们证明了所有三个光谱都存在于小型发电机中。在运动阶段,批量光谱发生在比湍流的能量携带尺度大的尺度上发生,并且在湍流的惯性范围内的较小尺度上的kazantsev光谱甚至对于磁性prandtl的统一数。在饱和状态下,发电机在大尺度上开发了一个saffman频谱,暗示了远程相关性的积累。在大型磁性prandtl数字下,在合成同步加速器发射图中可以看到细长的结构,显示了平均值,甚至E极化。我们还观察到E极化在亚抗性尺度上的E极化显着过多,并且在较大尺度上的缺陷。这一发现与在银河微波前景发射中观察到的过量观察到的发现不一致,这被认为与较大的尺度有关。 E和B极化可能是高度非高斯的,并且在发电机的运动学方面偏斜。然而,对于粉尘发射,偏振始终几乎是高斯,并且E极化中的过量较弱。
The magnetic fields in galaxy clusters and probably also in the interstellar medium are believed to be generated by a small-scale dynamo. Theoretically, during its kinematic stage, it is characterized by a Kazantsev spectrum, which peaks at the resistive scale. It is only slightly shallower than the Saffman spectrum that is expected for random and causally connected magnetic fields. Causally disconnected fields have the even steeper Batchelor spectrum. Here we show that all three spectra are present in the small-scale dynamo. During the kinematic stage, the Batchelor spectrum occurs on scales larger than the energy-carrying scale of the turbulence, and the Kazantsev spectrum on smaller scales within the inertial range of the turbulence -- even for a magnetic Prandtl number of unity. In the saturated state, the dynamo develops a Saffman spectrum on large scales, suggestive of the build-up of long-range correlations. At large magnetic Prandtl numbers, elongated structures are seen in synthetic synchrotron emission maps showing the parity-even E polarization. We also observe a significant excess in the E polarization over the parity-odd B polarization at subresistive scales, and a deficiency at larger scales. This finding is at odds with the observed excess in the Galactic microwave foreground emission, which is believed to be associated with larger scales. The E and B polarizations may be highly non-Gaussian and skewed in the kinematic regime of the dynamo. For dust emission, however, the polarized emission is always nearly Gaussian, and the excess in the E polarization is much weaker.