论文标题
X射线发射插入介质的动态加热:合并冲击和湍流耗散的作用
Dynamical heating of the X-ray emitting intracluster medium: the roles of merger shocks and turbulence dissipation
论文作者
论文摘要
星系簇内部的弥漫性等离子体具有几个keV的X射线发射温度。将这种内室内培养基(ICM)加热到这种温度的物理机制包括在星系群的外围的吸积冲击,由合并事件驱动的冲击以及某种忽略的机制 - 散热器内湍流的耗散。我们使用星系簇在omega500宇宙学模拟的拉格朗日示踪剂重新模拟中研究这些加热机制的相对作用。我们采用了一种新颖的分析方法,将温度升高分解为耗散加热和绝热加热的贡献。在这些加热速率的高分辨率时空图中,合并轨道清晰可见,表明合并事件在加热ICM中的主要作用。每次合并事件贡献的耗散加热时间都会扩大,并且在稀疏区域也发生在稀有区域,这表明通过耗散合并引起的湍流而加热的重要性。定量分析表明,湍流加热而不是在合并冲击时进行直接加热,主导了ICM的温度升高,尤其是在内部半径$ r <r <r _ {\ rm 500c} $下。此外,我们发现许多合并冲击几乎可以以几乎恒定的速度传播到非常大的半径$ r \ gg r _ {\ rm 500c} $,有些甚至可以触及并与积聚冲击并成为ICM的外部边界。总的来说,这些结果表明,如经典的平滑积聚图片所示,ICM以“内而外”的方式而不是``外面''加热。
The diffuse plasma inside clusters of galaxies has X-ray emitting temperatures of a few keV. The physical mechanisms that heat this intracluster medium (ICM) to such temperatures include the accretion shock at the periphery of a galaxy cluster, the shocks driven by merger events, as well as a somewhat overlooked mechanism -- the dissipation of intracluster turbulent motions. We study the relative role of these heating mechanisms using galaxy clusters in Lagrangian tracer particle re-simulations of the Omega500 cosmological simulation. We adopt a novel analysis method of decomposing the temperature increase at each time step into the contribution from dissipative heating and that from adiabatic heating. In the high-resolution spatial-temporal map of these heating rates, merger tracks are clearly visible, demonstrating the dominant role of merger events in heating the ICM. The dissipative heating contributed by each merger event is extended in time and also occurs in the rarefaction regions, suggesting the importance of heating by the dissipation of merger-induced turbulence. Quantitative analysis shows that turbulence heating, rather than direct heating at merger shocks, dominates the temperature increase of the ICM, especially at inner radii $r < r_{\rm 500c}$. In addition, we find that many merger shocks can propagate with almost constant velocity to very large radii $r \gg r_{\rm 500c}$, some even reach and join with the accretion shock and becoming the outer boundary of the ICM. Altogether, these results suggest that the ICM is heated more in an `inside-out' fashion rather than `outside-in' as depicted in the classical smooth accretion picture.