http://arxiv.org/abs/2210.08030
We present X-ray spectral analysis of XMM and Chandra observations in the 31.3 deg$^2$ Stripe-82X (S82X) field. Of the 6181 unique X-ray sources in this field, we select and analyze a sample of 2937 candidate active galactic nuclei (AGN) with solid redshifts and sufficient counts determined by simulations. Our results show an observed population with median values of spectral index $\Gamma=1.94_{-0.39}^{+0.31}$, column density log $N_H/\rm{cm}^{-2}=20.7_{-0.5}^{+1.2}$ ($21.6_{-0.9}^{+0.7}$ considering upper limits) and intrinsic, de-absorbed, 2-10 keV luminosity log $L_X/\rm{erg\,s}^{-1}=44.0_{-1.0}^{+0.7}$, in the redshift range 0-4. Correcting for observational biases, we derive the intrinsic, model-independent, fraction of AGN that are obscured ($22\leq\rm{log}\,N_H/\rm{cm}^{-2}<24$), finding a significant increase in the obscured AGN fraction with redshift and a decline with increasing luminosity. The average obscured AGN fraction is $57\pm4\%$ for log $L_X/\rm{erg\,s}^{-1}>43$. This work constrains the AGN obscuration and spectral shape of the still uncertain high-luminosity and high-redshift regimes (log $L_X/\rm{erg\,s}^{-1}>45.5$, $z>3$), where the obscured AGN fraction rises to $64\pm12\%$. The total, obscured, and unobscured X-ray luminosity functions (XLFs) are determined out to $z=4$. We report a luminosity and density evolution of the total XLF, with obscured AGN dominating at all luminosities at $z>2$ and unobscured sources prevailing at log $L_X/\rm{erg\,s}^{-1}>45$ at lower redshifts. Our results agree with the evolutionary models in which the bulk of AGN activity is triggered by gas-rich environments and in a downsizing scenario. Also, the black hole accretion density is found to evolve similarly to the star formation rate density, confirming the co-evolution scenario between AGN and host galaxy, but suggesting different time scales in their growing history.
A. Peca, N. Cappelluti, M. Urry, et. al.
Tue, 18 Oct 22
47/99
Comments: 30 pages, 35 figures, submitted to ApJ
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