2016MNRAS.459..585E


Query : 2016MNRAS.459..585E

2016MNRAS.459..585E - Mon. Not. R. Astron. Soc., 459, 585-594 (2016/June-2)

Disc outflows and high-luminosity true type 2 AGN.

ELITZUR M. and NETZER H.

Abstract (from CDS):

The absence of intrinsic broad-line emission has been reported in a number of active galactic nuclei (AGN), including some with high Eddington ratios. Such 'true type 2 AGN' are inherent to the disc-wind scenario for the broad-line region: broad-line emission requires a minimal column density, implying a minimal outflow rate and thus a minimal accretion rate. Here we perform a detailed analysis of the consequences of mass conservation in the process of accretion through a central disc. The resulting constraints on luminosity are consistent with all the cases where claimed detections of true type 2 AGN pass stringent criteria, and predict that intrinsic broad-line emission can disappear at luminosities as high as ∼4 x 1046 erg/s and any Eddington ratio, though more detections can be expected at Eddington ratios below ∼1 per cent. Our results are applicable to every disc outflow model, whatever its details and whether clumpy or smooth, irrespective of the wind structure and its underlying dynamics. While other factors, such as changes in spectral energy distribution or covering factor, can affect the intensities of broad emission lines, within this scenario they can only produce true type 2 AGN of higher luminosity then those prescribed by mass conservation.

Abstract Copyright: © 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): galaxies: active - galaxies: nuclei - quasars: emission lines - quasars: general

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 2dFGRS TGS564Z081 Sy2 01 19 08.6635573080 -34 11 30.527946780   16.226   15.275   ~ 91 0
2 MCG-01-05-031 Sy2 01 45 25.4701541520 -03 49 37.694192736   14 14 12.91   ~ 48 0
3 ATO J029.5198-00.8727 AGN 01 58 04.7506373016 -00 52 21.927742716   18.84 18.34     ~ 18 0
4 2MASS J08405813+3833003 Sy1 08 40 58.1463496344 +38 33 00.266798772   17.97 17.43     ~ 9 0
5 SDSS J091440.82+435715.7 G 09 14 40.8276264000 +43 57 15.721403292           ~ 4 0
6 NGC 3079 Sy2 10 01 57.8789863992 +55 40 47.449758324 11.57 11.54 10.86     ~ 1391 3
7 NGC 3147 Sy2 10 16 53.6388580752 +73 24 02.641798224   11.43 10.61     ~ 490 2
8 3XMM J104549.6+213106 X 10 45 49.63 +21 31 06.0           ~ 1 0
9 NGC 3660 Sy2 11 23 32.2781260536 -08 39 30.730097016   15.34 14.45     ~ 178 0
10 2MASS J11275821+5835587 EmG 11 27 58.249 +58 35 58.84       17.53   ~ 7 0
11 2XMM J121048.0+393745 AGN 12 10 48.0514363488 +39 37 45.410760156           ~ 7 0
12 2XMM J123103.2+110648 AG? 12 31 03.239 +11 06 48.60           ~ 46 0
13 PMN J1515+0421 rG 15 15 25.0475186040 +04 21 45.419956092   17       ~ 24 1
14 2MASX J19271951+6533539 Sy1 19 27 19.5393064368 +65 33 54.335877408     15.4     ~ 90 0
15 SDSS J213026.23-000204.7 G 21 30 26.231 -00 02 04.75           ~ 8 0
16 QSO B2131-427 Sy2 21 34 26.4 -42 29 58   20.20       ~ 17 0

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