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Broadband Spectral Energy Distributions of Active Galactic Nuclei from an Accretion Disk with Advective Coronal Flow

机译:具有正向冠状流的吸积盘中活动银河核的宽带光谱能量分布

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Recent multiwaveband observations of Seyfert nuclei and QSOs established significant deviations in the spectral shape of the big blue bump from a blackbody spectral shape; soft X-ray excess has a spectral index α (Fν ∝ ν-α) of 1.6 and hard X-ray tail with α of ~0.7. We construct a disk-corona model which accounts for such broadband spectral properties. We study the emission spectrum emerging from a vertical disk-corona structure composed of two-temperature plasma by solving hydrostatic equilibrium and radiative transfer self-consistently. A fraction f of viscous heating due to mass accretion is assumed to be dissipated in a corona with a Thomson optical depth of τc, where advective cooling is also included, and a remaining fraction, 1 - f, dissipates within a main body of the disk. Our model can nicely reproduce the soft X-ray excess with a power-law shape and the hard tail extending to ~50 keV. The different spectral slopes (α ~ 1.5 below 2 keV and ~0.5 above) are the results of different emission mechanisms and different sites; the former slope is due to unsaturated Comptonization from the innermost zone, and the latter is due to a combination of the Comptonization, bremsstrahlung, and a reflection of the coronal radiation at the disk-corona boundary from the inner to surrounding zone (≤300 Schwarzschild radii). The emergent optical spectrum is redder (α ~ 0.3) than that of the standard disk (α ~ -0.3), being consistent with observations, due to the different efficiencies of spectral hardening of disk emission at different radii. Further, we find that the cutoff frequency of the hard X-ray (~coronal electron temperature) and broadband spectral shape are insensitive to the black hole mass, while the peak frequency of the big blue bump is sensitive to the mass as the peak frequency ∝M.
机译:Seyfert核和QSOs最近的多波段观测结果表明,大蓝bump的光谱形状与黑体光谱形状之间存在显着偏差。软X射线过剩的光谱指数α(Fναν-α)为1.6,硬X射线尾部的α为〜0.7。我们构造了一个磁盘电晕模型,解释了这种宽带光谱特性。我们通过自洽地解决静水平衡和辐射传递,研究了由两温等离子体组成的垂直圆盘电晕结构产生的发射光谱。假定由于质量积聚而产生的粘性加热的分数f在Thomson光学深度为τc的电晕中消散,其中还包括对流冷却,而其余的1-f在磁盘主体内消散。我们的模型可以很好地重现具有幂律形状的软X射线多余部分,而硬尾部延伸到〜50 keV。不同的光谱斜率(低于2 keV时为α〜1.5,高于2 keV时为〜0.5)是不同发射机制和不同位置的结果。前者的斜率是由于来自最内层区域的不饱和康顿化,而后者是由于康普顿化,致辐射以及从内层到周围区域的圆盘电晕边界处日冕辐射的反射(≤300Schwarzschild)半径)。出射光谱比标准圆盘(α〜-0.3)偏红(α〜0.3),与观测值一致,这是由于在不同半径下圆盘发射光谱硬化的效率不同。此外,我们发现硬X射线的截止频率(〜冠状电子温度)和宽带光谱形状对黑洞质量不敏感,而大的蓝色凸点的峰值频率对质量敏感,即峰值频率∝M。

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