2019A&A...623A.172C


Query : 2019A&A...623A.172C

2019A&A...623A.172C - Astronomy and Astrophysics, volume 623A172-172 (2019/3-1)

X-ray emission of z > 2.5 active galactic nuclei can be obscured by their host galaxies.

CIRCOSTA C., VIGNALI C., GILLI R., FELTRE A., VITO F., CALURA F., MAINIERI V., MASSARDI M. and NORMAN C.

Abstract (from CDS):

We present a multiwavelength study of seven active galactic nuclei (AGN) at spectroscopic redshift >2.5 in the 7Ms Chandra Deep Field South that were selected for their good far-infrared (FIR) and submillimeter (submm) detections. Our aim is to investigate the possibility that the obscuration observed in the X-rays can be produced by the interstellar medium (ISM) of the host galaxy. Based on the 7Ms Chandra spectra, we measured obscuring column densities N_H, X_ in excess of 7x1022cm–2 and intrinsic X-ray luminosities LX>1044erg/s for our targets, as well as equivalent widths for the Fe Kα emission line EWrest≥0.5-1keV. We built the UV-to-FIR spectral energy distributions (SEDs) by using broadband photometry from the CANDELS and Herschel catalogs. By means of an SED decomposition technique, we derived stellar masses (M*∼1011M☉), IR luminosities (LIR>1012L☉), star formation rates (SFR∼190-1680M☉/yr) and AGN bolometric luminosities (Lbol∼1046erg/s) for our sample. We used an empirically calibrated relation between gas masses and FIR/submm luminosities and derived Mgas∼0.8-5.4x1010M☉. High-resolution (0.3-0.7'') ALMA data (when available, CANDELS data otherwise) were used to estimate the galaxy size and hence the volume enclosing most of the ISM under simple geometrical assumptions. These measurements were then combined to derive the column density associated with the ISM of the host, which is on the order of N_H, ISM_∼1023–24cm–2. The comparison between the ISM column densities and those measured from the X-ray spectral analysis shows that they are similar. This suggests that at least at high redshift, significant absorption on kiloparsec scales by the dense ISM in the host likely adds to or substitutes that produced by circumnuclear gas on parsec scales (i.e., the torus of unified models). The lack of unobscured AGN among our ISM-rich targets supports this scenario.

Abstract Copyright: © ESO 2019

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: star formation - quasars: general - surveys - X-rays: galaxies

Simbad objects: 12

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Number of rows : 12
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 [LBX2017] 42 Sy2 03 31 51.94 -27 53 27.2 26.57 25.14 25.38 24.74   ~ 62 0
2 [LBX2017] 170 AGN 03 32 07.99858 -27 46 57.2578   25.6308   24.931 25.0534 ~ 46 0
3 CXOCDFS J033218.9-275136 Sy2 03 32 18.8321 -27 51 35.476   25.15   24.51 25.128 ~ 83 0
4 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
5 ALESS J033229.29-275619.7 Sy1 03 32 29.2912 -27 56 19.465     26.76 25.82 25.1655 ~ 122 0
6 [VV2006] J033229.9-275106 Sy2 03 32 29.8487 -27 51 05.879   27.5675 25.05 23.970 24.5370 ~ 101 0
7 NAME Extended Chandra Deep Field South reg 03 32 30.0 -27 48 20           ~ 862 0
8 NAME BzK 4892 Sy2 03 32 35.73 -27 49 16.2   25.681 27.798 25.00 24.645 ~ 89 0
9 ACS-GC 90045073 Sy2 03 32 39.670 -27 48 50.60   27.3148   25.18 24.512 ~ 108 0
10 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
11 NGC 4102 Sy2 12 06 23.11513 +52 42 39.4160   11.8       ~ 449 1
12 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4

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