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arXiv 0903.0477astro-ph.HE
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磁支撑黑洞吸积盘的热平衡

Thermal Equilibria of Magnetically Supported, Black Hole Accretion Disks

H. Oda, M. Machida, K. E. Nakamura, R. Matsumoto

摘要:

我们提出了新的热平衡解决方案,光学薄和厚磁盘纳入磁场。本文的目的是解释亮硬态和亮/慢转变中观察到的爆发的上升阶段在BHC。在三维MHD模拟结果的基础上,我们假设圆盘内部的磁场是湍流的,并且由方位分量控制,并且方位平均Maxwell应力与总压力成正比。我们规定的磁通量平流率,以确定在一个给定的半径的方位角磁通量。我们发现磁支持,热稳定的解决方案,光学薄和厚的磁盘,其中加热增强的强磁场平衡的辐射冷却。低- $β$盘中的温度低于ADAF/RIAF中的温度,但高于标准盘中的温度。我们还研究了热平衡解的径向依赖性。光学薄,低$β$分支延伸到$ \dot M \gtrsim 0.1 {\dot M}_{\rm Edd}$,其中温度与质量吸积速率反相关。因此,光学薄的低$β$磁盘可以解释明亮的硬态。光学厚的低$β$圆盘具有有效温度$T_{\rm eff} \propto \varpi^{-3/4}$的径向依赖性.这样的盘将被观察为保持在高/软状态。此外,由于光学厚的低$β$分支与辐射压主导的标准盘分支相交,光学厚的低$β$盘和薄盘之间将发生极限环振荡。这些极限环振荡将表现出比标准盘和细长盘之间更小的光度变化。

英文摘要:

We present new thermal equilibrium solutions for optically thin and thick disks incorporating magnetic fields. The purpose of this paper is to explain the bright hard state and the bright/slow transition observed in the rising phases of outbursts in BHCs. On the basis of the results of 3D MHD simulations, we assume that magnetic fields inside the disk are turbulent and dominated by the azimuthal component and that the azimuthally averaged Maxwell stress is proportional to the total pressure. We prescribe the magnetic flux advection rate to determine the azimuthal magnetic flux at a given radius. We find magnetically supported, thermally stable solutions for both optically thin and thick disks, in which the heating enhanced by the strong magnetic field balances the radiative cooling. The temperature in a low-$β$ disk is lower than that in an ADAF/RIAF but higher than that in a standard disk. We also study the radial dependence of the thermal equilibrium solutions. The optically thin, low-$β$ branch extends to $ \dot M \gtrsim 0.1 {\dot M}_{\rm Edd}$, in which the temperature anti-correlates with the mass accretion rate. Thus optically thin low-$β$ disks can explain the bright hard state. Optically thick, low-$β$ disks have the radial dependence of the effective temperature $T_{\rm eff} \propto \varpi^{-3/4}$. Such disks will be observed as staying in a high/soft state. Furthermore, limit cycle oscillations between an optically thick low-$β$ disk and a slim disk will occur because the optically thick low-$β$ branch intersects with the radiation pressure dominated standard disk branch. These limit cycle oscillations will show a smaller luminosity variation than that between a standard disk and a slim disk.

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