论文标题

弓冲击的热发射II:Zeta Ophiuchi的3D磁性水力动力学模型

Thermal emission from bow shocks II: 3D magnetohydrodynamic models of Zeta Ophiuchi

论文作者

Green, S., Mackey, J., Kavanagh, P., Haworth, T. J., Moutzouri, M., Gvaramdaze, V. V.

论文摘要

附近的巨大,失控的恒星Zeta Ophiuchi在光学和红外线中检测到了大弓冲击,并且在Oplaway O恒星中独特地从震惊的恒星风中检测到了散射的X射线发射。在这里,我们对Zeta Ophiuchi的弓冲击进行了首次详细的计算研究,以测试弓形冲击的简单模型是否可以解释观察到的星云,并将检测到的X射线发射与模拟发射图进行比较。我们重新分配了档案{\ it chandra}观察弓击的震动风区的热弥散X射线发射,发现与对应于弥漫性亮度相对应的总未吸收X射线通量(0.3-2 keV频段) $ l_ \ mathrm {x} = 2.33〜(0.79-3.45)\ times10^{29} $ ergs $^{ - 1} $。 3D MHD模拟使用一系列由观察性约束动机的恒星和ISM参数对恒星风与均匀ISM的相互作用进行建模。从三个模拟中生成了合成红外,HA,软X射线,发射度量和GHz发射图,以与相关的观测值进行比较。模拟Zeta Ophiuchi的空间速度具有明显的径向速度产生的红外发射图具有与观测的更好一致的弓形冲击的开头,而不是完全在天空平面上运动的情况。压力最高的仿真具有最接近的匹配度,通量水平在观测下限的2倍以内,并且$ \ log_ {10}的排放加权温度(t_ \ mathrm {a}/\ mathrm {k})= 6.4 $,尽管散射发射的形态似乎有些不同。观察到的X射线发射是恒星附近最亮的气泡,而模拟预测随着密度的增加,接触性不连续性会变亮。

The nearby, massive, runaway star Zeta Ophiuchi has a large bow shock detected in optical and infrared, and, uniquely among runaway O stars, diffuse X-ray emission is detected from the shocked stellar wind. Here we make the first detailed computational investigation of the bow shock of Zeta Ophiuchi, to test whether a simple model of the bow shock can explain the observed nebula, and to compare the detected X-ray emission with simulated emission maps. We re-analysed archival {\it Chandra} observations of the thermal diffuse X-ray emission from the shocked wind region of the bow shock, finding total unabsorbed X-ray flux (0.3-2 keV band) corresponding to a diffuse luminosity of $L_\mathrm{X}=2.33~(0.79-3.45)\times10^{29}$ergs$^{-1}$. 3D MHD simulations were used to model the interaction of the star's wind with a uniform ISM using a range of stellar and ISM parameters motivated by observational constraints. Synthetic infrared, Ha, soft X-ray, emission measure, and radio 6\,GHz emission maps were generated from three simulations, for comparison with relevant observations. Simulations where the space velocity of Zeta Ophiuchi has a significant radial velocity produce infrared emission maps with opening angle of the bow shock in better agreement with observations than for the case where motion is fully in the plane of the sky. The simulation with the highest pressure has the closest match, with flux level within a factor of 2 of the observational lower limit, and emission weighted temperature of $\log_{10}(T_\mathrm{A}/\mathrm{K})=6.4$, although the morphology of the diffuse emission appears somewhat different. Observed X-ray emission is a filled bubble brightest near the star whereas simulations predict brightening towards the contact discontinuity as density increases.

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