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arXiv 1502.07353astro-ph.HE
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用NuSTAR确定康普顿厚活动星系核的覆盖因子

Determining the covering factor of Compton-thick active galactic nuclei with NuSTAR

M. Brightman, M. Balokovic, D. Stern, P. Arevalo, D. R. Ballantyne, F. E. Bauer, S. E. Boggs, W. W. Craig, F. E. Christensen, A. Comastri, F. Fuerst, P. Gandhi,… 展开作者

M. Brightman, M. Balokovic, D. Stern, P. Arevalo, D. R. Ballantyne, F. E. Bauer, S. E. Boggs, W. W. Craig, F. E. Christensen, A. Comastri, F. Fuerst, P. Gandhi, C. J. Hailey, F. A. Harrison, R. C. Hickox, M. Koss, S. LaMassa, S. Puccetti, E. Rivers, R. Vasudevan, D. J. Walton, W. W. Zhang

摘要:

与活动星系核(AGN)环面相关的康普顿厚遮蔽物质的覆盖因子目前最好通过X射线波段中沿视线($N_{H}>1.5\times10^{24}$ cm $^{-2}$)显示康普顿厚吸收的源的分数来理解,它揭示了平均覆盖因子。然而,由于极端的遮蔽,确定这种康普顿厚度的部分是困难的。由于其光谱覆盖在硬X射线($>$ 10 keV),NuSTAR对AGN覆盖因子敏感,因为X射线的康普顿散射在这些能量下占主导地位。本文对NuSTAR观测到的10个活动星系核进行了光谱分析,这些活动星系核的遮蔽介质对于康普顿散射来说是光学厚度的,称为康普顿厚度(CT)活动星系核。我们使用Brightman和Nandra的环面模型,该模型预测了环面中再处理的X射线光谱,并将环面张角作为自由参数,旨在分别确定这些源中康普顿厚气体的覆盖因子。在整个样品中,我们发现了从轻度到重度的康普顿厚度柱,$N_{H}$从$10^{24}-10^{26}$ cm $^{-2}$开始测量,覆盖因子范围很广,单个测量值范围为0.2-0.9。我们发现,覆盖因子,$f_{c}$,是一个强烈的内在2-10 keV的光度,$L_{X}$,其中$f_{c}=(-0.41\pm0.13)$日志$_{10}$($L_{X}$ /erg s $^{-1}$)$+18.31\pm5.33$,在$L_{X}$(10 $^{41.5}-10^{44}$ erg s $^{-1}$)超过两个数量级的递减函数。这里测量的覆盖因子与用$L_{X}>10^{42.5}$ erg s $^{-1}$研究局部活动星系核所确定的作为$L_{X}$函数的遮蔽分数吻合得很好。

英文摘要:

The covering factor of Compton-thick obscuring material associated with the torus in active galactic nuclei (AGN) is at present best understood through the fraction of sources exhibiting Compton-thick absorption along the line of sight ($N_{H}>1.5\times10^{24}$ cm$^{-2}$) in the X-ray band, which reveals the average covering factor. Determining this Compton-thick fraction is difficult however, due to the extreme obscuration. With its spectral coverage at hard X-rays ($>$10 keV), NuSTAR is sensitive to the AGN covering factor since Compton scattering of X-rays off optically thick material dominates at these energies. We present a spectral analysis of 10 AGN observed with NuSTAR where the obscuring medium is optically thick to Compton scattering, so called Compton-thick (CT) AGN. We use the torus models of Brightman & Nandra which predict the X-ray spectrum from reprocessing in a torus and include the torus opening angle as a free parameter and aim to determine the covering factor of the Compton-thick gas in these sources individually. Across the sample we find mild to heavy Compton-thick columns, with $N_{H}$ measured from $10^{24}-10^{26}$ cm$^{-2}$, and a wide range of covering factors, where individual measurements range from 0.2-0.9. We find that the covering factor, $f_{c}$, is a strongly decreasing function of the intrinsic 2-10 keV luminosity, $L_{X}$, where $f_{c}=(-0.41\pm0.13)$log$_{10}$($L_{X}$/erg s$^{-1}$)$+18.31\pm5.33$, across more than two orders of magnitude in $L_{X}$ (10$^{41.5}-10^{44}$ erg s$^{-1}$). The covering factors measured here agree well with the obscured fraction as a function of $L_{X}$ as determined by studies of local AGN with $L_{X}>10^{42.5}$ erg s$^{-1}$.

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