2021ApJ...919..108K


Query : 2021ApJ...919..108K

2021ApJ...919..108K - Astrophys. J., 919, 108-108 (2021/October-1)

The nature of jets in double-peaked emission-line AGN in the KISSR sample.

KHARB P., SUBRAMANIAN S., DAS M., VADDI S. and PARAGI Z.

Abstract (from CDS):

Double-peaked emission-line AGN (DPAGN) have been regarded as binary black hole candidates. We present here results from parsec-scale radio observations with the Very Long Baseline Array (VLBA) of five DPAGN belonging to the KISSR sample of emission-line galaxies. This work concludes our pilot study of nine type 2 Seyfert and LINER DPAGN from the KISSR sample. In the nine sources, dual compact cores are only detected in the "offset AGN," KISSR 102. However, the overall incidence of jets in the eight sources that were detected with the VLBA is >=60%. We find a difference in the "missing flux density" going from the Very Large Array to VLBA scales between Seyferts and LINERs, with LINERs showing less missing flux density on parsec-scales. Using the emission-line modeling code, MAPPINGS III, we find that the emission lines are likely to be influenced by jets in 5/9 sources. Jet-medium interaction is the likely cause of the emission-line splitting observed in the SDSS spectra of these sources. Jets in radio-quiet AGN are therefore energetically capable of influencing their parsec- and kpc-scale environments, which makes them agents of "radio AGN feedback" (similar to radio-loud AGN).

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Seyfert galaxies

CDS comments: N1 and N2 in Figure 1 are not in SIMBAD.

Simbad objects: 15

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Number of rows : 15
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SDSS J013815.05+002914.0 QSO 01 38 15.0512581440 +00 29 14.009377992   20.40 20.01     ~ 28 0
2 [VV98] J115016.5+433205 QSO 11 50 16.60280297 +43 32 05.9063832     20.30 19.28   ~ 46 1
3 2MASX J11563290+4259392 Sy2 11 56 32.8675248696 +42 59 39.319156176   16.30 15.54     ~ 11 0
4 NGC 4135 Sy2 12 09 08.8089458664 +44 00 11.324839788   14.79 14.02     ~ 45 0
5 6C 122432+435742 QSO 12 26 57.9042742008 +43 40 58.448863668   19.70 19.53 18.5   ~ 51 1
6 2MASX J12303157+4258219 Sy2 12 30 31.5964900752 +42 58 22.269950400   17.36 16.41     ~ 17 0
7 LEDA 1847714 LIN 12 41 35.1153 +28 50 36.271   17.37 16.24     ~ 18 1
8 2MASX J13132589+4332148 Sy2 13 13 25.8542057616 +43 32 14.853545952   18.45 17.43     ~ 39 0
9 2MASX J14034502+2921441 Sy2 14 03 45.0344737584 +29 21 43.920817416   16.09 15.23     ~ 26 0
10 7C 145225.0+300803 QSO 14 54 32.29788050 +29 55 58.0563178   18.2 18.5 18.9   ~ 65 1
11 2MASX J15022874+2858152 Sy2 15 02 28.7681484864 +28 58 15.530503152   16.56 15.66     ~ 12 0
12 ICRF J153939.1+274438 Bla 15 39 39.13713864 +27 44 38.2113620   19.13 18.76 17.29   ~ 100 1
13 2MASX J15500978+2911068 LIN 15 50 09.8042287008 +29 11 07.235472228   16.58 15.68     ~ 19 0
14 ICRF J160533.0+300129 QSO 16 05 33.04805145 +30 01 29.7027995   20.73 20.42 19.94   ~ 42 1
15 2MASX J16063176+2927568 LIN 16 06 31.7812805184 +29 27 56.927122704   17.28 16.22     ~ 9 0

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