Bibcode
Tozzi, P.; Gilli, R.; Mainieri, V.; Norman, C.; Risaliti, G.; Rosati, P.; Bergeron, J.; Borgani, S.; Giacconi, R.; Hasinger, G.; Nonino, M.; Streblyanska, A.; Szokoly, G.; Wang, J. X.; Zheng, W.
Bibliographical reference
Astronomy and Astrophysics, Volume 451, Issue 2, May IV 2006, pp.457-474
Advertised on:
5
2006
Journal
Citations
358
Refereed citations
323
Description
We present a detailed X-ray spectral analysis of the sources in the 1Ms
catalog of the Chandra Deep Field South (CDFS) taking advantage of
optical spectroscopy and photometric redshifts for 321 extragalactic
sources out of the total sample of 347 sources. As a default spectral
model, we adopt a power law with slope Γ with an intrinsic
redshifted absorption N_H, a fixed Galactic absorption and an unresolved
Fe emission line. For 82 X-ray bright sources, we are able to perform
the X-ray spectral analysis leaving both Γ and NH free.
The weighted mean value for the slope of the power law is < Γ
> ≃ 1.75 ± 0.02, and the distribution of best fit values
shows an intrinsic dispersion of σ_int ≃ 0.30. We do not find
hints of a correlation between the spectral index Γ and the
intrinsic absorption column density N_H. We then investigate the
absorption distribution for the whole sample, deriving the NH
values in faint sources by fixing Γ = 1.8. We also allow for the
presence of a scattered component at soft energies with the same slope
of the main power law, and for a pure reflection spectrum typical of
Compton-thick AGN. We detect the presence of a scattered soft component
in 8 sources; we also identify 14 sources showing a reflection-dominated
spectrum. The latter are referred to as Compton-thick AGN candidates. By
correcting for both incompleteness and sampling-volume effects, we
recover the intrinsic NH distribution representative of the
whole AGN population, f(N_H) dN_H, from the observed one. f(N_H) shows a
lognormal shape, peaking around log(N_H)≃ 23.1 and with σ
≃ 1.1. Interestingly, such a distribution shows continuity between
the population of Compton-thin and that of Compton-thick AGN. We find
that the fraction of absorbed sources (with N_H>1022
cm-2) in the sample is constant (at the level of about 75%)
or moderately increasing with redshift. Finally, we compare the optical
classification to the X-ray spectral properties, confirming that the
correspondence of unabsorbed (absorbed) X-ray sources to optical type I
(type II) AGN is accurate for at least 80% of the sources with spectral
identification (1/3 of the total X-ray sample).