Broadband Spectral Modeling of the M87 Nucleus

Andrzej Niedźwiecki, Michał Szanecki and Agnieszka Janiuk
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Abstract

We study spectra produced by weakly accreting black hole (BH) systems using the semianalytic advection-dominated accretion flow (ADAF) model and the general-relativistic magnetohydrodynamic (GRMHD) simulation. We find significant differences between these two approaches related to a wider spread of the flow parameters as well as a much steeper radial distribution of the magnetic field in the latter. We apply these spectral models to the broadband spectral energy distribution (SED) of the nucleus of the M87 galaxy. The standard (in particular, 1D) formulation of the ADAF model does not allow us to explain it; previous claims that this model reproduces the observed SED suffer from an inaccurate treatment of the Compton process. The spectra based on GRMHD simulation are in a much better agreement with the observed data. In our GRMHD model, in which we assumed the BH spin a = 0.9, the bulk of radiation observed between the millimeter and the X-ray range is produced in the disk area within 4 gravitational radii from the BH. In this solution, the synchrotron component easily reproduces the spectral data between the millimeter and the UV range, and the Compton component does not violate the X-rays constraints, for yr−1 and a relatively strong magnetic field, with the plasma β ∼ 1 in the region where radiation is produced. However, the Compton component cannot explain the observed X-ray spectrum. Instead, the X-ray spectrum can be reproduced by a high-energy tail of the synchrotron spectrum if electrons have a hybrid energy distribution with a ∼5% nonthermal component.
M87 核的宽带光谱建模
我们利用半解析吸积流(ADAF)模型和广义相对论磁流体动力学(GRMHD)模拟,研究了弱吸积黑洞(BH)系统产生的光谱。我们发现这两种方法存在明显差异,前者的流动参数分布更广,后者的磁场径向分布更陡峭。我们将这些光谱模型应用于 M87 星系核的宽带光谱能量分布(SED)。ADAF模型的标准(特别是一维)表述并不能让我们解释它;以前声称该模型可以再现观测到的SED,是因为对康普顿过程的处理不准确。基于 GRMHD 模拟的光谱与观测数据的一致性要好得多。在我们的 GRMHD 模型中,我们假定 BH 自旋 a = 0.9,在毫米和 X 射线范围内观测到的大部分辐射都产生于距离 BH 4 个引力半径范围内的盘区。在这个方案中,同步辐射成分很容易再现毫米波和紫外波段之间的光谱数据,而康普顿成分也没有违反 X 射线约束条件,即在年-1 和相对较强的磁场条件下,辐射产生区域的等离子体 β ∼ 1。然而,康普顿成分无法解释观测到的 X 射线光谱。相反,如果电子具有混合能量分布,其中有 ∼5% 的非热量成分,那么同步辐射光谱的高能量尾部就可以再现 X 射线光谱。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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