2006ApJ...652..112C


Query : 2006ApJ...652..112C

2006ApJ...652..112C - Astrophys. J., 652, 112-119 (2006/November-3)

A physical model for active galactic nuclei with double-peaked broad emission lines.

CAO X. and WANG T.-G.

Abstract (from CDS):

The double-peaked broad emission lines are usually thought to be linked to accretion disks; however, the local viscous heating in the line-emitting disk portion is usually insufficient for the observed double-peaked broad-line luminosity in most sources. It was suggested that the X-ray radiation from an ion-supported torus in the inner region of the disk can photoionize the outer line-emitting disk region. However, our calculations show that only a small fraction (≲2.3%) of the radiation from the radiatively inefficient accretion flow (RIAF) in the inner region of the disk can photoionize the line-emitting disk portion, because the solid angle of the outer disk portion subtended to the inner region of the RIAF is too small. We propose a physical model for double-peaked line emitters, in which only those AGNs with sufficient matter above the disk (slowly moving jets or outflows) can scatter enough photons radiated from the inner disk region to the outer line-emitting disk portion extending from several hundred to more than 2000 gravitational radii. Our model predicts a power-law r-dependent line emissivity εHα∝R–βd, where β∼2.5, which is consistent with β∼2-3 required by the model fittings for double-peaked line profiles. Using a sample of radio-loud AGNs with double-peaked emission lines, we show that the outer disk regions can be efficiently illuminated by the photons scattered from slow or mild relativistic electron-positron jets with γj≲2. It is consistent with the fact that no double-peaked emission line is present in strong radio quasars with relativistic jets. For radio-quiet double-peaked line emitters, slow outflows with Thomson scattering depth∼0.2 instead of jets can scatter sufficient photons to (illuminate) the line-emitting regions. This model can therefore solve the energy budget problem for double-peaked line emitters.

Abstract Copyright: ∼

Journal keyword(s): Accretion, Accretion Disks - Galaxies: Active - Galaxies: Quasars: Emission Lines

Simbad objects: 20

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Number of rows : 20
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 ICRF J003820.5-020740 Sy1 00 38 20.52934376 -02 07 40.5469964   19.04 18.02 17.6   ~ 255 1
2 4C 31.06 QSO 01 57 15.3287506728 +31 54 19.021353048     18.9     ~ 42 2
3 7C 020415.59+291722.00 Sy1 02 07 02.2064405304 +29 30 46.051043400   16 16     ~ 161 1
4 LEDA 1230840 Sy1 02 38 32.6708623272 +02 33 49.093335396     17.7     ~ 38 0
5 ESO 416-5 Sy1 02 38 45.1459401792 -30 48 23.394294000   14.98 14.85 14.14   ~ 63 0
6 LEDA 2823643 Sy1 03 42 05.4065822945 -37 03 21.576616433   18.84 18.6 17.65   ~ 44 1
7 3C 93.0 BLL 03 43 29.9963486496 +04 57 48.612170988   18.49 18.14     ~ 155 1
8 LEDA 88364 Sy2 04 52 35.8822730880 -18 12 01.876652208   17.8       ~ 36 0
9 ESO 252-18A Sy1 05 19 49.7229323856 -45 46 43.852662732   15.73 15.77 14.85   ~ 714 0
10 ICRF J074541.6+314256 Sy1 07 45 41.6715742128 +31 42 56.614217508   16.10 15.97     ~ 265 1
11 CBS 74 Sy1 08 32 25.3533620280 +37 07 36.254235468   16.46 16.37     ~ 90 0
12 ICRF J092338.8-213547 Bla 09 23 38.8852056768 -21 35 47.129767764   13.0   12.80   ~ 99 1
13 PKS 1020-10 BLL 10 22 32.8200967176 -10 37 44.309640648   16.25 16.11 16.0   ~ 144 1
14 6C 142125+510933 Bla 14 23 14.1852096840 +50 55 37.285758732   18.25 17.88 14.93   ~ 96 1
15 ICRF J144302.7+520137 Sy1 14 43 02.76069031 +52 01 37.2985156   18.96 18.29     ~ 316 3
16 3C 332.0 Sy1 16 17 42.5380089648 +32 22 34.372277976   18.25 17.45     ~ 268 1
17 Z 252-40 Bla 17 19 14.4925971408 +48 58 49.423205136   15.86 14.81 9.44   ~ 335 1
18 Z 173-14 Sy1 18 35 03.3896172576 +32 41 46.855964616   16.50 15.39 10.50   ~ 688 1
19 3C 390.3 Bla 18 42 08.9904975672 +79 46 17.127835104   16.06 15.38     ~ 1381 1
20 QSO B1914-45 BLL 19 17 39.6365228976 -45 30 30.769741764   17.01 16.80     ~ 32 1

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