论文标题

X射线红移,用于遮盖的AGN:J1030深场上的案例研究

X-ray redshifts for obscured AGN: a case study in the J1030 deep field

论文作者

Peca, Alessandro, Vignali, Cristian, Gilli, Roberto, Mignoli, Marco, Nanni, Riccardo, Marchesi, Stefano, Bolzonella, Micol, Brusa, Marcella, Cappelluti, Nico, Comastri, Andrea, Lanzuisi, Giorgio, Vito, Fabio

论文摘要

我们提出了一个程序,以限制基于低计算统计的X射线光谱的活动($ n_h> 10^{22} $ cm $^{ - 2} $)主动的银河核(AGN),当光度和/或光谱杂物无法获得时,可以在光度和/或光谱杂点时采用。我们在Chandra Deep Field($ \ sim $ 479 ks,335 Arcmin $^2 $)中选择了54个模糊的AGN候选样品,$ hr> -0.1 $,$ hr> -0.1 $,围绕$ z = 6.3 $ z = 6.3 $ QSO SDSS J1030+0524。该样本的中位数为$ \ of $ \ of bow80 $净计数,在0.5-7 kev Energy Band中。我们估计可靠的X射线红移解决方案利用了晦涩的AGN光谱中的主要特征,例如Fe 6.4 kev k $ \mathrmα$发射线,7.1 keV Fe吸收边缘和光电吸收率。通过光谱模拟研究了此类特征的重要性,然后将衍生的X射线红移溶液与光度红移进行比较。光度法和X射线红移均针对33个来源得出。当通过任何方法得出多个溶液时,我们发现将两种技术的红移溶液组合起来会提高RMS的两个因子。使用我们的红移估算($ 0.1 \ Lessim z \ Lessim 4 $),我们在范围内得出了吸收列密度$ \ sim 10^{22} -10^{24} $ cm $^{ - 2} $ and prosptignt-cm $^{ - 2} $,并吸收率和2-10 Kev Rest-Frame luminosities,2-10 Kev Rest-Frame $ \ sim $ \ sim $ \ sim 10^45}^42}^42}^42^42}} s $^{ - 1} $,中位值$ n_h = 1.7 \ times 10^{23} $ cm $^{ - 2} $和$ l _ {\ mathrm {2-10 \,kev}} = 8.3 \ times10^\ times10^{43} $ erg s $ s $^{43} $。我们的结果表明,所采用的程序可以应用于当前和将来的X射线调查,对于仅在X射线中检测到的来源或具有不确定的光度或单线光谱红移的来源。

We present a procedure to constrain the redshifts of obscured ($N_H > 10^{22}$ cm$^{-2}$) Active Galactic Nuclei (AGN) based on low-count statistics X-ray spectra, which can be adopted when photometric and/or spectroscopic redshifts are unavailable or difficult to obtain. We selected a sample of 54 obscured AGN candidates on the basis of their X-ray hardness ratio, $HR>-0.1$, in the Chandra deep field ($\sim$479 ks, 335 arcmin$^2$) around the $z=6.3$ QSO SDSS J1030+0524. The sample has a median value of $\approx80$ net counts in the 0.5-7 keV energy band. We estimate reliable X-ray redshift solutions taking advantage of the main features in obscured AGN spectra, like the Fe 6.4 keV K$\mathrmα$ emission line, the 7.1 keV Fe absorption edge and the photoelectric absorption cut-off. The significance of such features is investigated through spectral simulations, and the derived X-ray redshift solutions are then compared with photometric redshifts. Both photometric and X-ray redshifts are derived for 33 sources. When multiple solutions are derived by any method, we find that combining the redshift solutions of the two techniques improves the rms by a factor of two. Using our redshift estimates ($0.1\lesssim z \lesssim 4$), we derived absorbing column densities in the range $\sim 10^{22}-10^{24}$ cm$^{-2}$ and absorption-corrected, 2-10 keV rest-frame luminosities between $\sim 10^{42}$ and $10^{45}$ erg s$^{-1}$, with median values of $N_H = 1.7 \times 10^{23}$ cm$^{-2}$ and $L_{\mathrm{2-10\, keV}} = 8.3\times10^{43}$ erg s$^{-1}$, respectively. Our results suggest that the adopted procedure can be applied to current and future X-ray surveys, for sources detected only in the X-rays or that have uncertain photometric or single-line spectroscopic redshifts.

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