2011MNRAS.416..917C


Query : 2011MNRAS.416..917C

2011MNRAS.416..917C - Mon. Not. R. Astron. Soc., 416, 917-926 (2011/September-2)

On the origin of radio loudness in active galactic nuclei and its relationship with the properties of the central supermassive black hole.

CHIABERGE M. and MARCONI A.

Abstract (from CDS):

We investigate the relationship between the mass of central supermassive black holes (SMBHs) and the radio loudness of active galactic nuclei (AGNs). We use the most recent calibrations to derive `virial' BH masses for samples of radio-loud quasi-stellar objects (QSOs) for which relatively small masses (MBH< 108 M☉) have been estimated in the literature. We take into account the effect of radiation pressure on the broad-line region (BLR) which reduces the `effective' gravitational potential experienced by the broad-line clouds and affects the mass estimates of bright quasars. We show that in well-defined samples of nearby low-luminosity AGNs (LLAGNs), QSOs and AGNs from the Sloan Digital Sky Survey, radio-loud AGNs invariably host SMBHs exceeding ∼108 M☉. On the other hand, radio-quiet AGNs are associated with a much larger range of BH masses. The overall result still holds even without correcting the BH mass estimates for the effects of radiation pressure. We present a conjecture based on these results, which aims at explaining the origin of radio loudness in terms of two fundamental parameters: the spin of the BH and the BH mass. We speculate that in order to produce a radio-loud AGN, both of the following requirements must be satisfied: (1) the BH mass, MBH, has to be larger than ∼108 M☉, and (2) the spin of the BH must be significant, in order to satisfy theoretical requirements. Taking into account the most recent observations, we envisage a scenario in which the merger history of the host galaxy plays a fundamental role in accounting for both the properties of the AGN and the galaxy morphology, which in our picture are strictly linked. On the one hand, radio-loud sources might be obtained only through major `dry' mergers involving BH of large mass, which would give rise to both the `core' morphology and the significant BH spin needed. On the other hand, radio-quiet AGNs might reside in galaxies that underwent different evolutionary paths, depending on their BH mass.

Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: fundamental parameters - galaxies: nuclei

Simbad objects: 41

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Number of rows : 41
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 IRAS 00321-0018 Sy2 00 34 43.5012933672 -00 02 27.032963604   16.26 15.67     ~ 50 1
2 RX J0117.4+0742 Sy2 01 17 27.0317528075 +07 41 47.447209038   18.0       ~ 44 0
3 LEDA 88588 Sy1 07 08 41.4886614696 -49 33 06.308921700   16.02 15.7 12.7   ~ 566 0
4 7C 074905.70+460420.00 BLL 07 52 44.2077683088 +45 56 57.426578736   17.95 16.93     ~ 125 1
5 NVSS J075444+354712 rG 07 54 44.0841433128 +35 47 12.753832164   19.78 19.24     ~ 9 1
6 2MASX J08304516+3709465 Sy2 08 30 45.2159033424 +37 09 46.811978316   18.54 17.88     ~ 14 0
7 SDSS J085010.42+074758.5 Sy1 08 50 10.4287335000 +07 47 58.546785912   18.38 17.69     ~ 9 1
8 IRAS F09005+0223 Sy2 09 03 07.84032 +02 11 52.0620   20.86 19.90     ~ 29 1
9 6C 090251+464619 Bla 09 06 15.53979871 +46 36 19.0241852   16.80 16.08     ~ 63 1
10 SDSS J092936.75+571149.7 Sy2 09 29 36.754 +57 11 49.79   20.29 19.75     ~ 2 0
11 5C 1.33 Bla 09 37 12.32736501 +50 08 52.0975584   19.51 18.94 18.88   ~ 158 1
12 6C 093652+511701 Sy2 09 40 03.7670725992 +51 04 21.801075924   19.03 18.17     ~ 9 1
13 NVSS J094525+352103 rG 09 45 25.9005678048 +35 21 03.561543864   19.37 18.65     ~ 33 1
14 2MASS J10041087+5230251 Sy1 10 04 10.8447240816 +52 30 25.298476560   20.14 19.43     ~ 22 0
15 4C 52.22 BLL 10 31 43.5166048176 +52 25 35.090452452   19.71 18.83     ~ 26 1
16 2MASS J10333068+0704071 Sy1 10 33 30.6529078015 +07 04 07.310646893   19.36 18.69     ~ 2 0
17 2dFGRS TGN362Z241 Sy2 10 39 15.6964510296 -00 39 16.903925424   17.93 17.45     ~ 18 1
18 IRAS 10378+1109 Sy1 10 40 29.1640944744 +10 53 18.202070076   17.79 17.18     ~ 115 1
19 ICRF J110845.4+020240 BLL 11 08 45.48841189 +02 02 40.9040661   19.45 18.61 16.558   ~ 68 1
20 2dFGRS TGN370Z068 Sy1 11 18 07.4803587144 +00 27 34.967317896   19.68 18.71 16.851   ~ 27 0
21 87GB 115136.0+025423 BLL 11 54 09.2858650004 +02 38 15.138384342   19.91 19.04 17.7   ~ 24 1
22 SDSS J115437.43+114858.9 Sy1 11 54 37.4334589008 +11 48 58.957642620   19.89 19.55     ~ 14 0
23 87GB 121944.6+583113 BLL 12 22 09.3010840296 +58 14 21.448956588   19.17 18.46     ~ 18 1
24 2MASS J12465124+1509142 Sy1 12 46 51.24432 +15 09 14.2920   20.22 19.35     ~ 3 0
25 4C 49.25 BLL 12 47 07.3205733336 +49 00 17.883948492   20.08 19.20     ~ 44 1
26 SDSS J130633.05+002248.4 Sy2 13 06 33.065 +00 22 48.00   19.89 19.13 17.095   ~ 13 0
27 MCG-06-30-015 Sy1 13 35 53.7691256160 -34 17 44.160716796   13.89 13.61 8.9   ~ 1559 0
28 SDSS J135646.10+102609.0 Sy2 13 56 46.106 +10 26 09.09   18.90 18.11     ~ 95 0
29 IRAS 14041+0117 Sy2 14 06 38.1987435120 +01 02 54.571253496   18.71 18.25     ~ 30 0
30 2MASX J14223792+0448487 Sy1 14 22 37.9122280920 +04 48 48.589542864   18.48 17.85     ~ 10 0
31 2MASS J14434155+3835222 Sy1 14 43 41.5414042992 +38 35 21.875642952   18.44 17.88     ~ 9 1
32 2MASS J15151355+5525042 Sy1 15 15 13.5937761648 +55 25 04.212163308   19.79 18.75     ~ 4 0
33 Z 21-63 BLL 15 16 40.21905672 +00 15 01.9090936   17.28 16.64 10.53   ~ 217 1
34 2MASX J15552206+2813227 Sy2 15 55 22.0443251400 +28 13 23.211233652   19.10 18.26     ~ 17 0
35 2MASX J16332357+4718588 Sy1 16 33 23.5812109560 +47 18 58.936241628   17.77 17.35     ~ 88 1
36 SDSS J164126.90+432121.5 Sy2 16 41 26.9054262216 +43 21 21.588876756   20.22 19.48     ~ 17 0
37 QSO J1644+2619 Bla 16 44 42.5339200680 +26 19 13.227002976   18.80 18.42     ~ 114 1
38 3C 390.3 Bla 18 42 08.9904975672 +79 46 17.127835104   16.06 15.38     ~ 1381 1
39 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
40 2MASS J21185296-0732275 Sy1 21 18 52.9632528816 -07 32 27.590693424   20.07 19.48     ~ 62 1
41 IRAS 21497-0824 Sy1 21 52 26.0010437592 -08 10 24.888907308   15.43 14.91 14.58   ~ 43 1

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