Hamiltonian formulation of relativistic magnetohydrodynamic accretion on a general spherically symmetric and static black hole: quantum effects on shock states
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Abstract
In this paper, our aim is to extend our earlier work [Ahmed et al. in Eur. Phys. J. C 76:280, 2016], investigating an axisymmetric plasma flow with angular momentum onto a spherical black hole. To accomplish that goal, we focus on the case in which the ideal magnetohydrodynamic approximation is valid, utilizing certain conservation laws which arise from particular symmetries of the system. After formulating a Hamiltonian of the physical system, we solve the Hamilton equations and look for critical solutions of (both in and out) flows. Reflecting the difference from the Schwarzschild spacetime, the positions of sonic points (fast magnetosonic point, slow magnetosonic point, Alfvén point) are altered. We explore several kinds of flows including critical, non-critical, global, magnetically arrested and shock induced. Lastly, we analyze the shock states near a specific quantum corrected Schwarzschild black hole and determine that quantum effects do not favor shock states by pushing the shock location outward.
在本文中,我们的目的是扩展我们的早期工作[Ahmed 等人,载于 Eur. Phys. J. C 76:280, 2016],研究球形黑洞上带有角动量的轴对称等离子体流。为了实现这一目标,我们重点研究了理想磁流体力学近似有效的情况,并利用了由系统特定对称性产生的某些守恒定律。在提出物理系统的哈密顿方程后,我们求解哈密顿方程,并寻找(流入和流出)流的临界解。为了反映与施瓦兹柴尔德时空的差异,声波点(快磁声波点、慢磁声波点、阿尔芬点)的位置发生了变化。我们探讨了几种流动,包括临界流、非临界流、全局流、磁阻流和冲击诱导流。最后,我们分析了特定量子修正的施瓦兹柴尔德黑洞附近的冲击态,并确定量子效应不会通过将冲击位置向外推而有利于冲击态。
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