论文标题

关于超级埃德丁顿的硬性X射线光子指数与积聚率之间的关系

On the relation between hard X-ray photon index versus accretion rate for super-Eddington accreting quasars

论文作者

Huang, Jian, Luo, Bin, Du, Pu, Hu, Chen, Wang, Jian-Min, Li, Yi-Jia

论文摘要

我们调查了超级X射线光子指数($γ$)与超级 - 埃德丁顿的积分类星体相关的相关性是否不同于埃德丁顿的积分类星体。我们从斯隆数字天空调查数据发布14个类星体目录中构建了113个明亮的类星体样本,其中包括38个类星体作为Super-Eddington子样本和75个类星体作为子埃德丁顿子样本。我们使用基于$ {\ rmhβ} $线的简单 - 直期病毒质量公式来得出黑洞质量,我们使用标准的薄磁盘模型来得出我们的样品的无尺寸增强率($ \ dot {\ dot {\ nathscr {m}} $)。这些类星体的X射线数据是从Chandra和XMM-Newton档案中收集的。我们使用单个幂律模型符合硬X射线光谱,以获得$γ$值。我们发现一个具有统计学意义的($ r _ {\ rm s} = 0.43 $,$ p = 7.75 \ times {10}^{ - 3} $)$γ$和$γ$和$ \ dot {\ nathscr {\ mathscr {m Mathscr {m Mathscr {m}} $的相关性。 $γ$ - $ \ dot {\ mathscr {m}} $相关性的相关性也很重要,但较弱($ r _ {\ rm s} = 0.30 $,$ p = 9.98 \ times {10}}}}^{ - 3} $)。线性回归分析表明,$ {\rmγ} =(0.34 \ pm0.11){\ rm log} {\ dot {\ dot {\ mathscr {m}}}}}+(1.71 \ pm0.17)$ and $ {\ rmγ} =(\ rmγ} =(0.09 \ pm09 \ pm09 \ pm0.0.04) log} {\ dot {\ mathscr {m}}}}+(1.93 \ pm0.04)$分别用于超级和子埃德丁顿子样本。 $γ$ - $ \ dot {\ mathscr {m}} $相关性的两个子样本不同,这表明这两种类型的系统中的磁盘 - corona连接不同。我们提出了一个定性的解释,即在超级 - 埃德丁顿制度中的陡峭$γ$ - $ \ dot {\ mathscr {m}} $相关性,其中涉及从超级埃德丁顿(Super-Eddington Quassars)中厚的厚磁盘从厚磁盘中收到的较大种子光子通量。

We investigate whether the hard X-ray photon index ($Γ$) versus accretion rate correlation for super-Eddington accreting quasars is different from that for sub-Eddington accreting quasars. We construct a sample of 113 bright quasars from the Sloan Digital Sky Survey Data Release 14 quasar catalog, including 38 quasars as the super-Eddington subsample and 75 quasars as the sub-Eddington subsample. We derive black-hole masses using a simple-epoch virial mass formula based on the ${\rm Hβ}$ lines, and we use the standard thin disk model to derive the dimensionless accretion rates ($\dot{\mathscr{M}}$) for our sample. The X-ray data for these quasars are collected from the Chandra and XMM-Newton archives. We fit the hard X-ray spectra using a single power-law model to obtain $Γ$ values. We find a statistically significant ($R_{\rm S}=0.43$, $p=7.75\times{10}^{-3}$) correlation between $Γ$ and $\dot{\mathscr{M}}$ for the super-Eddington subsample. The $Γ$-$\dot{\mathscr{M}}$ correlation for the sub-Eddington subsample is also significant, but weaker ($R_{\rm S}=0.30$, $p=9.98\times{10}^{-3}$). Linear regression analysis shows that ${\rm Γ}=(0.34\pm0.11){\rm log}{\dot{\mathscr{M}}}+(1.71\pm0.17)$ and ${\rm Γ}=(0.09\pm0.04){\rm log}{\dot{\mathscr{M}}}+(1.93\pm0.04)$ for the super- and sub-Eddington subsamples, respectively. The $Γ$-$\dot{\mathscr{M}}$ correlations of the two subsamples are different, suggesting different disk-corona connections in these two types of systems. We propose one qualitative explanation of the steeper $Γ$-$\dot{\mathscr{M}}$ correlation in the super-Eddington regime that involves larger seed photon fluxes received by the compact coronae from the thick disks in super-Eddington accreting quasars.

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