首页> 外文期刊>The Astrophysical journal >QUASI-PERIODIC INWARD SHOCK FORMATIONS IN THE SYSTEM OF A BLACK HOLE AND AN ACCRETION DISK AND APPLICATION TO QUASI-PERIODIC OSCILLATIONS IN GALACTIC BLACK HOLE CANDIDATES
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QUASI-PERIODIC INWARD SHOCK FORMATIONS IN THE SYSTEM OF A BLACK HOLE AND AN ACCRETION DISK AND APPLICATION TO QUASI-PERIODIC OSCILLATIONS IN GALACTIC BLACK HOLE CANDIDATES

机译:黑洞和增生盘系统中的准周期向内激波形成及其在银黑洞候选群的准周期振荡中的应用

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We performed 1.5-dimensional general relativistic hydrodynamic simulations with a Kerr metric to construct a model for high-frequency quasi-periodic oscillations (QPOs) in microquasars. The simulations were performed assuming an initial accretion disk without viscosity rotating around a Kerr black hole at sub-Keplerian velocity (sub-Keplerian case), which induces various wave modes everywhere in the disk. We found that quasi-periodic inward shock waves propagate from the accretion disk toward the black hole. The frequency of the shock formation is about the maximum epicyclic frequency in the disk (κ_(max)), which depends on the rotation of the black hole. In order to understand the mechanism of the shock formation, we also performed a simulation assuming an initial linear perturbation injected at one point in the Keplerian disk (linear perturbation case) and found an oscillation with frequency ~κ at the point where the perturbation injection occurred. To explain the simulation result, we derived an analytic solution for the time evolution of the linear perturbation of physical variables near the point of the perturbation injection and found that the time evolution of the oscillation can be described well. From comparison of the result in the sub-Keplerian case with that of the linear perturbation case, we found that the periodicity of the quasi-periodic shock formation in the sub-Keplerian case is due to a filtering effect by the epicyclic frequency distribution in the disk, which acts on the wave propagation toward the black hole. The only necessary condition for quasi-periodic shock formation is having a nonsteady character for the disks, which can be a source of acoustic waves. The frequency of the shock formation (~κ_(max)) is on the order of the frequency of the high-frequency QPOs in microquasars and depends on the rotation of the black hole. Hence, we can estimate the spin parameter (a) of a black hole candidate (BHC) in a microquasar by comparing the frequency of the high-frequency QPO with κ_(max). The spin parameters of the BHCs in microquasars are roughly estimated to be a = 0.345 ± 0.345 for GRS 1915+105 and a = 0.895 ± 0.105 for GRO J1655-40.
机译:我们使用Kerr量度进行了1.5维广义相对论流体动力学模拟,以构建微类星体中的高频准周期振荡(QPO)模型。进行模拟时,假设初始吸积盘没有以亚开普勒速度绕克尔黑洞旋转(亚开普勒情况),从而在盘中到处产生各种波动模式。我们发现准周期向内激波从吸积盘传播到黑洞。冲击形成的频率大约是圆盘中最大周转频率(κ_(max)),这取决于黑洞的旋转。为了理解激波形成的机理,我们还进行了模拟,假设在开普勒圆盘的某一点处注入了初始线性扰动(线性扰动情况),并且在发生扰动注入的点处发现了一个频率约为κ的振荡。 。为了解释仿真结果,我们推导了在扰动注入点附近的物理变量的线性扰动的时间演化的解析解,发现可以很好地描述振荡的时间演化。通过比较次开普勒情形和线性摄动情形的结果,我们发现,在次开普勒情形中准周期冲击形成的周期性是由于周向频率分布中的周波频率分布的滤波作用所致。盘,它作用于波向黑洞传播。准周期震动形成的唯一必要条件是磁盘具有不稳定特性,而磁盘可能是声波的来源。冲击形成的频率(〜κ_(max))约为微类星体中高频QPO的频率,并取决于黑洞的旋转。因此,我们可以通过比较高频QPO的频率和κ_(max)来估计微类星体中黑洞候选(BHC)的自旋参数(a)。粗略估计类星体中BHC的自旋参数对于GRS 1915 + 105为a = 0.345±0.345,对于GRO J1655-40为a = 0.895±0.105。

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