2022ApJ...936...73A


Query : 2022ApJ...936...73A

2022ApJ...936...73A - Astrophys. J., 936, 73 (2022/September-1)

Dependence of the Radio Emission on the Eddington Ratio of Radio-quiet Quasars.

ALHOSANI A., GELFAND J.D., ZAW I., LAOR A., BEHAR E., CHEN S. and WRZOSEK R.

Abstract (from CDS):

Roughly 10% of quasars are “radio-loud,” producing copious radio emission in large jets. The origin of the low-level radio emission seen from the remaining 90% of quasars is unclear. Observing a sample of eight radio-quiet quasars with the Very Long Baseline Array, we discovered that their radio properties depend strongly on their Eddington ratio rEdd ≡ LAGN/LEdd. At lower Eddington ratios rEdd ≲ 0.3, the total radio emission of the AGN predominately originates from an extremely compact region, possibly as small as the accretion disk. At higher Eddington ratios (rEdd ≳ 0.3), the relative contribution of this compact region decreases significantly, and though the total radio power remains about the same, the emission now originates from regions ≳100 pc in size. The change in the physical origin of the radio-emitting plasma region with rEdd is unexpected, as the properties of radio-loud quasars show no dependence with Eddington ratio. Our results suggest that at lower Eddington ratios the magnetized plasma is likely confined by the accretion disk corona and only at higher Eddington ratios escapes to larger scales. Stellar-mass black holes show a similar dependence of their radio properties on the accretion rate, supporting the paradigm that unifies the accretion onto black holes across the mass range.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Active galactic nuclei - Radio active galactic nuclei - Radio quiet quasars

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 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
2 MITG J0054+2549 Rad 00 54 36.12 +25 50 04.3           ~ 3 0
3 LEDA 3237 Sy1 00 54 52.1183662680 +25 25 38.983241532     15.42     ~ 421 0
4 [VV2006] J005503.5+140806 QSO 00 55 03.5227428120 +14 08 06.538324524   19.96 19.70     ~ 27 1
5 4C 39.25 Bla 09 27 03.01394144 +39 02 20.8518067   17.17 17.00 16.486   ~ 1036 1
6 LEDA 37161 Sy1 11 52 03.5494748736 -11 22 24.091043304   13.7 15.5 12.5   ~ 138 0
7 QSO B1150-1048 QSO 11 53 22.3140976104 -11 05 12.587211816           ~ 28 1
8 6C 143651+372332 Bla 14 38 53.61097349 +37 10 35.4166935       19.11   ~ 98 1
9 Mrk 478 Sy1 14 42 07.4714418744 +35 26 22.938625500   14.91 14.58     ~ 567 1
10 ICRF J161042.0+241449 Bla 16 10 42.02677563 +24 14 49.0115848   20.79 20.33 19.24   ~ 45 1
11 Mrk 876 Sy1 16 13 57.1795021224 +65 43 09.952685328   16.03 15.49     ~ 620 0
12 Ton 256 Sy1 16 14 13.2050129832 +26 04 16.221218880   16.06 16.50     ~ 282 1
13 [VV96] J162304.5+662401 Bla 16 23 04.52169655 +66 24 01.0787041   19.477   17.430   ~ 67 1
14 3C 345 Bla 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1808 3
15 8C 2007+777 BLL 20 05 30.9987913056 +77 52 43.248139536     16.5 17.36   ~ 474 1
16 ICRF J213016.2+084355 QSO 21 30 16.24974988 +08 43 55.9275702           ~ 17 0
17 Mrk 1513 Sy1 21 32 27.8162556672 +10 08 19.252365396   14.92 14.64     ~ 651 0
18 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2
19 ICRF J230040.8+033710 QSO 23 00 40.88579354 +03 37 10.8399514   20.0 20.0     ~ 28 1
20 LEDA 70504 Sy1 23 07 02.9147133288 +04 32 57.101475624   16.32 15.50     ~ 135 0

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