2021A&A...654A..94M


Query : 2021A&A...654A..94M

2021A&A...654A..94M - Astronomy and Astrophysics, volume 654A, 94-94 (2021/10-1)

The H I absorption zoo: JVLA extension to z ∼ 0.4.

MURTHY S., MORGANTI R., OOSTERLOO T. and MACCAGNI F.M.

Abstract (from CDS):

We present an HI 21 cm absorption study of a sample of 26 radio-loud active galactic nuclei (AGN) at 0.25 < z < 0.4 carried out with the Karl G. Jansky Very Large Array. Our aim was to study the rate of incidence of HI in different classes of radio AGN, the morphology and kinematics of the detected HI, and the nature of the interaction between the HI and the radio source at these redshifts. Our sample consists of 14 sources with sizes of up to tens of kpc and 12 compact sources (< a few kpc) in the radio-power range 1025.7 W Hz–1-1026.5 W Hz–1. We detect HI in five sources, corresponding to a detection rate of ∼19%. Within the error bars, this agrees with the detection rate found at lower redshifts. We find that the rest-frame UV luminosities of most of the sources in the sample, including all the detections, are below the proposed threshold above which the HI is supposed to have been ionised. An analysis of the optical emission-line spectra of the sources shows that despite their high radio powers, about one-third of the sample, including two detections, are low-ionisation sources. The radio continuum emission from the sources detected in HI is unresolved at ∼5 to 10 kpc scales in our observations, but shows extended structure on parsec scales. We analysed the HI 21 cm absorption spectra of the detections to understand the morphology and kinematics of HI. The absorption profiles are mostly complex with widths between the nulls ranging from ∼60 km s–1 to 700 km s–1. These detections also exhibit remarkably high HI column densities in the range ∼1021 cm–2-1022 cm–2 for Tspin = 100 K and unit covering factor. Our modelling of the HI 21 cm absorption profiles suggests that in two sources the gas appears to be disturbed, and in three cases, including one with disturbed HI, the majority of the absorption is consistent with it arising from an HI disc. Despite the high radio power of our sources, we do not detect fast outflows. However, the optical emission lines in these detections show the presence of significantly disturbed gas in the nuclear regions in the form of very wide and highly blueshifted emission-line components. Since some of our detections are also low-ionisation AGN, it is quite possible that this disturbance is caused by the radio jets. Overall, our findings point towards a continuation of the low-z trends in the HI detection rate and the incidence of HI in radio AGN up to z∼0.4.

Abstract Copyright: © ESO 2021

Journal keyword(s): galaxies: active - galaxies: ISM - radio lines: galaxies

Simbad objects: 35

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Number of rows : 35
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 87GB 002823.5+005914 BiC 00 30 58.304 +01 15 59.70     20.0     ~ 6 1
2 NGC 1167 LIN 03 01 42.3322774176 +35 12 20.300948892   13.84 12.77     ~ 355 2
3 3C 84 Sy2 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4007 3
4 NVSS J075621+355441 rG 07 56 21.7692859488 +35 54 42.119317224           ~ 8 1
5 NVSS J083824+371036 rG 08 38 25.0106220120 +37 10 36.596070300           ~ 10 1
6 ICRF J085450.5+621850 Sy1 08 54 50.57629150 +62 18 50.1927118     19.00 17   ~ 43 1
7 87GB 085914.2+031623 G 09 01 50.966 +03 04 23.00     19.0     ~ 10 1
8 4C 39.32 rG 10 28 44.2728990384 +38 44 36.859285032   18.4       ~ 47 1
9 4C 19.35 Rad 11 06 55.2688359264 +19 09 12.358127124   20.0 19.0     ~ 11 1
10 SDSSCGB 9178.1 G 11 11 40.800 +35 53 36.52           ~ 2 0
11 2MASS J11234189+1252139 G 11 23 41.90352 +12 52 13.9404           ~ 1 0
12 4C 16.31 Rad 11 24 34.7791407384 +16 16 51.791510208   19.5 20.0     ~ 7 1
13 NVSS J112833+324322 rG 11 28 33.0329 +32 43 22.634           ~ 10 1
14 ICRF J114408.7+005436 Sy2 11 44 08.71379962 +00 54 36.3361900     19.4     ~ 24 1
15 ICRF J114538.5+442021 Sy2 11 45 38.51859906 +44 20 21.9141720   18.79 18.15     ~ 28 1
16 LB 2136 Sy1 11 53 24.46663994 +49 31 08.8301372   17.94 17.66     ~ 498 1
17 ICRF J123413.3+475351 Sy1 12 34 13.3306496760 +47 53 51.237796812   17.62 17.31 16.8   ~ 83 1
18 NAME Centaurus A Sy2 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4483 3
19 NVSS J140416+411748 rG 14 04 16.3566607536 +41 17 48.737495544           ~ 13 1
20 NVSS J140854+302103 rG 14 08 54.087 +30 21 03.39           ~ 5 1
21 2MASS J14290409+0251399 G 14 29 04.1 +02 51 40     18.5     ~ 10 1
22 2MASS J14523938+0627382 Sy1 14 52 39.3867 +06 27 38.154           ~ 17 1
23 87GB 145106.9+041149 BiC 14 53 38.478 +03 59 33.35           ~ 9 1
24 ICRF J145844.7+372021 BLL 14 58 44.7945139728 +37 20 21.622681212   20.30 19.81 19.43   ~ 87 1
25 ICRF J145859.3+041613 Sy1 14 58 59.35621394 +04 16 13.8204121   19.09 18.55 18.6   ~ 74 1
26 NVSS J150719+364246 Rad 15 07 19.5321 +36 42 45.335           ~ 5 1
27 ICRF J152502.9+110744 Sy1 15 25 02.93423158 +11 07 44.0632453   20.20 19.50     ~ 50 1
28 87GB 153441.2+463731 Sy2 15 36 17.3377652184 +46 27 33.749602416   21.19 20.30     ~ 12 1
29 SDSS J162213.89+090421.4 QSO 16 22 13.8941747856 +09 04 21.402358356           ~ 4 1
30 ICRF J164733.5+270558 G 16 47 33.59838989 +27 05 58.2933151           ~ 15 1
31 87GB 165341.7+233354 Sy2 16 55 47.363 +23 29 30.52           ~ 6 1
32 ICRF J172109.4+354216 Sy1 17 21 09.49105029 +35 42 16.0634973   17.5   16.90   ~ 84 1
33 NAME Cyg A Sy2 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2367 2
34 ICRF J231635.1+040518 Sy2 23 16 35.1933566880 +04 05 18.297101076   17.54 16.68 17.220   ~ 294 1
35 ICRF J234106.9+001833 Sy2 23 41 06.90995266 +00 18 33.3367251   20.26 19.46 15.6   ~ 51 2

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