2019MNRAS.484..385V


Query : 2019MNRAS.484..385V

2019MNRAS.484..385V - Mon. Not. R. Astron. Soc., 484, 385-408 (2019/March-3)

A VLA-GMRT look at 11 powerful FR II quasars.

VADDI S., KHARB P., DALY R.A., O'DEA C.P., BAUM S.A., DEO D.K., BARBUSCA T.C. and MURALI C.

Abstract (from CDS):

We present results from 1.4 and 5 GHz observations at matched resolution with the Karl G. Jansky Very Large Array (VLA) of 11 powerful 3C FR II quasars. We examine the 11 quasars along with a sample of 13 narrow-line FR II radio galaxies and find that radio-loud unification largely holds but environmental effects cannot be ignored. The radio core prominence, largest linear size, and axial ratio parameter values indicate that quasars are at relatively smaller angles compared to the radio galaxies and thus probe orientation. Lack of correlation between statistical orientation indicators such as misalignment angle and radio core prominence, and larger lobe distortions in quasars compared to radio galaxies suggest that intrinsic/environment effects are also at play. Some of 150 MHz observations with the TGSS-GMRT reveal peculiar lobe morphologies in these FR II sources, suggesting complex past lives and possibly restarted AGN activity. Using the total 150 MHz flux density we estimate the time-averaged jet kinetic power in these sources and this ranges from (1-38) x 1045 erg s–1, with 3C 470 having the highest jet kinetic power.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): techniques: interferometric - galaxies: active - galaxies: high-redshift - quasars: general - radio continuum: galaxies

Simbad objects: 25

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Number of rows : 25
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 3C 6.1 BLL 00 16 31.12832880 +79 16 50.1722040   22       ~ 129 1
2 3C 13 rG 00 34 14.555 +39 24 16.67   22.5       ~ 144 1
3 2C 44 QSO 00 36 06.4449136608 +18 37 59.099054268   20 20     ~ 121 1
4 3C 34.0 rG 01 10 18.665 +31 47 20.48   21       ~ 177 2
5 3C 41.0 rG 01 26 44.388 +33 13 11.22   21       ~ 172 1
6 3C 44 rG 01 31 21.618 +06 23 43.24   21       ~ 66 1
7 2E 437 Sy1 01 36 24.4208152464 +20 57 27.522990972   18.15 18.10     ~ 367 2
8 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
9 3C 54.0 rG 01 55 30.164 +43 45 55.44   22.0       ~ 91 1
10 ICRF J041340.3+111214 Sy2 04 13 40.34100355 +11 12 14.7860055   18.96 18.01     ~ 334 1
11 3C 114 rG 04 20 22.104 +17 53 54.82   22       ~ 72 2
12 3C 142.1 rG 05 31 29.427 +06 30 25.58   21       ~ 83 1
13 3C 169.1 rG 06 51 15.356 +45 09 26.21   20.5       ~ 63 1
14 3C 172 rG 07 02 08.30458800 +25 13 53.5192680   20.5       ~ 121 1
15 3C 204 QSO 08 37 45.0013678200 +65 13 35.305376376   18.76 18.21     ~ 184 1
16 3C 205 Sy1 08 39 06.5324936736 +57 54 17.069000688   18.10 17.62     ~ 264 1
17 3C 208 QSO 08 53 08.6093021736 +13 52 54.845406984   17.76 17.42     ~ 257 1
18 [OKM2018] SWIFT J1104.8+7689 Sy1 11 04 13.8611496720 +76 58 58.194549084   15.70 15.72 15.40   ~ 564 1
19 ICRF J113957.0+654749 Sy1 11 39 57.0254367168 +65 47 49.483232880   16.50 16.32     ~ 528 1
20 4C 23.43 Bla 16 24 39.0838297968 +23 45 12.223370412   17.91 17.47     ~ 343 1
21 8C 1704+608 Bla 17 04 41.3742408840 +60 44 30.520617000   15.65 15.40 15.30   ~ 782 1
22 3C 432.0 QSO 21 22 46.3251704424 +17 04 37.916198832   18.18 17.96     ~ 215 2
23 3C 441 rG 22 06 04.917 +29 29 20.01   21.0       ~ 198 3
24 3C 469.1 rG 23 55 22.89 +79 55 21.0   22.5       ~ 85 2
25 3C 470.0 rG 23 58 35.340 +44 04 38.89   22.5       ~ 114 1

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