具有强磁化超爱丁顿吸积盘的黑洞射流反馈和自旋演化的配方

Angelo Ricarte, R. Narayan, B. Curd
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引用次数: 1

摘要

一个自旋黑洞(BH)从一个由强磁化等离子体组成的圆盘中通过一个被磁性捕获的圆盘吸积,已知会产生一个由BH的自旋能量驱动的有效电磁射流。我们提出了磁阻系统的广义相对论辐射磁流体动力学模拟,涵盖了亚至超爱丁顿吸积速率的范围。利用这些模拟的数值结果,我们开发了一个公式来描述吸积黑洞的磁化、射流效率和自旋演化作为其自旋和吸积速率的函数。接近爱丁顿吸积的黑洞会经历轻微的自旋下降,因为通过喷流的角动量损失,导致在爱丁顿极限下的平衡自旋为0.8而不是1.0。随着吸积速率在爱丁顿以上的增加,自旋下降效应变得越来越强,最终与先前基于非辐射模拟的预测趋同。特别是,自旋演化将高度超爱丁顿系统推向接近零的黑洞自旋。这封信中开发的公式可以应用于包括黑洞在内的星系和宇宙尺度的模拟。如果磁阻盘吸积在超大质量黑洞中是常见的,那么目前的结果对活动星系核反馈和宇宙自旋演化具有广泛的意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Recipes for Jet Feedback and Spin Evolution of Black Holes with Strongly Magnetized Super-Eddington Accretion Disks
A spinning black hole (BH) accreting from a disk of strongly magnetized plasma via a magnetically arrested disk is known to produce an efficient electromagnetic jet powered by the BH’s spin energy. We present general relativistic radiative magnetohydrodynamic simulations of magnetically arrested systems covering a range of sub- to super-Eddington accretion rates. Using the numerical results from these simulations, we develop formulae to describe the magnetization, jet efficiency, and spin evolution of an accreting BH as a function of its spin and accretion rate. A BH with near-Eddington accretion experiences a mild degree of spin-down because of angular momentum loss through the jet, leading to an equilibrium spin of 0.8 rather than 1.0 at the Eddington limit. As the accretion rate increases above Eddington, the spin-down effect becomes progressively stronger, ultimately converging on previous predictions based on nonradiative simulations. In particular, spin evolution drives highly super-Eddington systems toward a BH spin near zero. The formulae developed in this letter may be applied to galaxy- and cosmological-scale simulations that include BHs. If magnetically arrested disk accretion is common among supermassive BHs, the present results have broad implications for active galactic nucleus feedback and cosmological spin evolution.
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