Mateusz A. Ogrodnik, M. Hanasz, D. Wóltański, A. Gawryszczak
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引用次数: 0
摘要
在电磁辐射的射电范围内,在许多边缘星系中观测到由Comic Ray (CR)电子引起的星系外流和扩展的非热辐射,使我们能够估计星系磁场的强度和垂直结构。基于NGC891的观测特征,我们构建了该星系的全球模型。我们假设在大尺度上,被磁化的ISM的动力学是由宇宙射线驱动的。我们应用粗粒度动量有限体积(CGMV)来求解PIERNIK MHD代码“宇宙射线能谱”(CRESP)模块中CR电子的Fokker-Planck CR输运方程,以模拟CR在该星系中的传播。宇宙射线的整体传播由福克-普朗克方程描述。数值模型显示了cr驱动发电机对磁场的放大。我们通过改变注入光谱斜率,CR电子扩散系数和SFR的大小和动量依赖性来对系统进行参数研究。我们考虑了平流、扩散和绝热变化以及同步加速器和逆康普顿损失。同步辐射光谱、极化图和光谱指数图很好地再现了观测到的真实边缘星系的结构。不同模型的比较表明,CR𝑒−注入光谱较硬,SN→CR能量的转化率较高(10 - 20%),扩散系数为~ 9 × 10 28 cm 2 s−1。
Modeling CR electron propagation with PIERNIK & CRESP: simulations vs. observational data of NGC891
Galactic outflows and extended non-thermal emission due to Comic Ray (CR) electrons have been observed in many edge-on galaxies in the radio range of electromagnetic radiation, allowing us to estimate the strength and vertical structure of the galactic magnetic field. We construct a global model of NGC891 based on the observational characteristics of this galaxy. We assume that on large scales, the dynamics of the magnetized ISM is driven by Cosmic Rays. We apply the coarse-grained momentum finite volume (CGMV), for solving the Fokker–Planck CR transport equation for CR electrons in ”Cosmic Ray Energy SPectrum” (CRESP) module of PIERNIK MHD code to model CR propagation in this galaxy. The overall propagation of cosmic rays is described by the Fokker-Planck equation. The numerical model exhibits magnetic field amplification by CR-driven dynamo. We perform a parameter study of the system by varying the injection spectrum slope, the magnitude and momentum dependence of the CR electron diffusion coefficients and SFR. We take into account the advection, diffusion, and adiabatic changes as well as synchrotron and inverse-Compton losses. The spectrum of synchrotron radiation, polarization maps and spectral index maps reproduce the observed structures of the real edge-on galaxy very well. Comparison of different models suggests harder CR 𝑒 − injection spectra, higher conversion ratios of SN → CR energies (of 10–20%) and diffusion coefficients ∼ 9 × 10 28 cm 2 s − 1 .