2017MNRAS.466.2294R


Query : 2017MNRAS.466.2294R

2017MNRAS.466.2294R - Mon. Not. R. Astron. Soc., 466, 2294-2301 (2017/April-1)

On the efficiency of jet production in FR II radio galaxies and quasars.

RUSINEK K., SIKORA M., KOZIEL-WIERZBOWSKA D. and GODFREY L.

Abstract (from CDS):

Jet powers in many radio galaxies with extended radio structures appear to exceed their associated accretion luminosities. In systems with very low accretion rates, this is likely due to the very low accretion luminosities resulting from radiatively inefficient accretion flows. In systems with high accretion rates, the accretion flows are expected to be radiatively efficient, and the production of such powerful jets may require an accretion scenario, which involves magnetically arrested discs (MADs). However, numerical simulations of the MAD scenario indicate that jet production efficiency is large only for geometrically thick accretion flows and scales roughly with (H/R)2, where H is the disc height and R is the distance from the black hole. Using samples of FR II radio galaxies and quasars accreting at moderate accretion rates, we show that their jets are much more powerful than predicted by the MAD scenario. We discuss possible origins of this discrepancy, suggesting that it can be related to approximations adopted in magnetohydrodynamic simulations to treat optically thick accretion flow within the MAD zone, or may indicate that accretion discs are geometrically thicker than the standard theory predicts.

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

Journal keyword(s): acceleration of particles - radiation mechanisms: non-thermal - galaxies: jets - galaxies: jets

Simbad objects: 33

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Number of rows : 33
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 4C 25.01 Bla 00 19 39.7806511920 +26 02 52.277853012     15.4 15.04   ~ 110 1
2 ICRF J003820.5-020740 Sy1 00 38 20.52934376 -02 07 40.5469964   19.04 18.02 17.6   ~ 255 1
3 4C 11.06 BLL 00 44 34.9649859840 +12 11 12.050439000   20.5 19     ~ 42 1
4 3C 22.0 Sy1 00 50 56.21976 +51 12 03.3552   22.0       ~ 153 1
5 4C 29.02 Sy1 01 13 24.2416856760 +29 58 16.025424636     17.00     ~ 89 1
6 4C 31.06 QSO 01 57 15.3287506728 +31 54 19.021353048     18.9     ~ 42 2
7 ICRF J020213.6-762003 Sy1 02 02 13.6936269168 -76 20 03.062287464   16.95 16.90     ~ 111 1
8 7C 020415.59+291722.00 Sy1 02 07 02.2064405304 +29 30 46.051043400   16 16     ~ 161 1
9 4C 10.06 Sy1 02 17 07.6653021240 +11 04 09.877412784     16.46     ~ 105 1
10 7C 022118.10+273638.00 Sy1 02 24 12.2865158736 +27 50 11.538285648   19.502 18 18.263   ~ 210 1
11 PKS 0236+02 Rad 02 38 36.4 +02 34 35           ~ 7 0
12 ESO 416-5 Sy1 02 38 45.1459401792 -30 48 23.394294000   14.98 14.85 14.14   ~ 63 0
13 QSO J0311-7651 BLL 03 11 55.2496997640 -76 51 50.848335324 15.27 16.09 16.10 15.33   ~ 231 1
14 2MASX J03122653+3916298 Sy1 03 12 26.5935301344 +39 16 29.806577112     18.2     ~ 58 3
15 LEDA 2823643 Sy1 03 42 05.4065822945 -37 03 21.576616433   18.84 18.6 17.65   ~ 44 1
16 3C 111 Sy1 04 18 21.2772425736 +38 01 35.801359968   19.75 18.05     ~ 1002 2
17 QSO B0558-5026 BLL 05 59 47.3916612936 -50 26 52.025952120   15.18 14.97     ~ 307 1
18 3C 175.1 rG 07 14 04.682 +14 36 21.99   21.5       ~ 102 2
19 SDSS J073729.73+401955.8 BiC 07 37 29.738 +40 19 55.87           ~ 6 0
20 3C 184 rG 07 39 24.465 +70 23 10.91   21.5       ~ 140 1
21 NVSS J080107+435030 rG 08 01 07.9204921872 +43 50 30.498920916           ~ 11 1
22 NVSS J081734+445852 rG 08 17 34.4639332464 +44 58 50.867784840           ~ 15 1
23 SDSS J084813.17+570004.3 Sy2 08 48 13.1713779024 +57 00 04.313562192   20.54 19.57     ~ 11 0
24 4C 56.17 LIN 09 01 50.3195639400 +55 55 27.450956244           ~ 16 0
25 3C 268.1 rG 12 00 20.53 +73 00 45.7   22       ~ 149 1
26 7C 125441.29+473632.00 SyG 12 56 57.485 +47 20 20.23   22.0       ~ 285 1
27 3C 289 QSO 13 45 26.699 +49 46 31.39   23       ~ 161 1
28 Z 21-63 BLL 15 16 40.21905672 +00 15 01.9090936   17.28 16.64 10.53   ~ 217 1
29 ICRF J163433.8+624535 Sy2 16 34 33.80623119 +62 45 35.8960467   21.06 20.61     ~ 220 1
30 2MASX J16584721+6256245 rG 16 58 47.1579405600 +62 56 24.607158900           ~ 10 0
31 NVSS J172027+591343 rG 17 20 28.3182732072 +59 13 41.761328592           ~ 16 1
32 3C 356 QSO 17 24 20.232 +50 57 14.47   21.5 21.5     ~ 225 1
33 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0

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