2019A&A...623A..29F


Query : 2019A&A...623A..29F

2019A&A...623A..29F - Astronomy and Astrophysics, volume 623A, 29-29 (2019/3-1)

Hidden or missing outflows in highly obscured galaxy nuclei?

FALSTAD N., HALLQVIST F., AALTO S., KONIG S., MULLER S., ALADRO R., COMBES F., EVANS A.S., FULLER G.A., GALLAGHER J.S., GARCIA-BURILLO S., GONZALEZ-ALFONSO E., GREVE T.R., HENKEL C., IMANISHI M., IZUMI T., MANGUM J.G., MARTIN S., PRIVON G.C., SAKAMOTO K., VEILLEUX S. and VAN DER WERF P.P.

Abstract (from CDS):


Context. Understanding the nuclear growth and feedback processes in galaxies requires investigating their often obscured central regions. One way to do this is to use (sub)millimeter line emission from vibrationally excited HCN (HCN-vib), which is thought to trace warm and highly enshrouded galaxy nuclei. It has been suggested that the most intense HCN-vib emission from a galaxy is connected to a phase of nuclear growth that occurs before the nuclear feedback processes have been fully developed.
Aims. We aim to investigate if there is a connection between the presence of strong HCN-vib emission and the development of feedback in (ultra)luminous infrared galaxies ((U)LIRGs).
Methods. We collected literature and archival data to compare the luminosities of rotational lines of HCN-vib, normalized to the total infrared luminosity, to the median velocities of 119µm OH absorption lines, potentially indicating outflows, in a total of 17 (U)LIRGs.
Results. The most HCN-vib luminous systems all lack signatures of significant molecular outflows in the far-infrared OH absorption lines. However, at least some of the systems with bright HCN-vib emission have fast and collimated outflows that can be seen in spectral lines at longer wavelengths, including in millimeter emission lines of CO and HCN (in its vibrational ground state) and in radio absorption lines of OH.
Conclusions. We conclude that the galaxy nuclei with the highest LHCN–vib/LIR do not drive wide-angle outflows that are detectable using the median velocities of far-infrared OH absorption lines. This is possibly because of an orientation effect in which sources oriented in such a way that their outflows are not along our line of sight also radiate a smaller proportion of their infrared luminosity in our direction. It could also be that massive wide-angle outflows destroy the deeply embedded regions responsible for bright HCN-vib emission, so that the two phenomena cannot coexist. This would strengthen the idea that vibrationally excited HCN traces a heavily obscured stage of evolution before nuclear feedback mechanisms are fully developed.

Abstract Copyright: © ESO 2019

Journal keyword(s): galaxies: evolution - galaxies: nuclei - galaxies: ISM - ISM: molecules - ISM: jets and outflows

Simbad objects: 28

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Number of rows : 28
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 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1168 1
2 QSO J0457-2324 QSO 04 57 03.1791422424 -23 24 52.021129572   18.85 18.5 16.56   ~ 396 1
3 LEDA 17155 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 498 0
4 ESO 362-21 Sy1 05 22 57.98464178 -36 27 30.8512953   15.26 14.62 14.48   ~ 834 2
5 NAME IRAS F08572+3915 NW LIN 09 00 25.364 +39 03 54.23     16.66     ~ 420 1
6 UGC 5101 Sy2 09 35 51.6045544584 +61 21 11.589382368   15.20 15.50     ~ 572 4
7 NAME NGC 3690 East AGN 11 28 33.07 +58 33 54.2   11.8       ~ 631 4
8 LEDA 39024 LIN 12 13 46.107 +02 48 41.50           ~ 354 1
9 6dFGS gJ122503.9-064053 LIN 12 25 03.8941406496 -06 40 52.501670544   15.53       ~ 68 0
10 NGC 4355 Sy2 12 26 54.6206739120 -00 52 39.421212996   14.21 13.37     ~ 491 2
11 QSO J1246-0730 QSO 12 46 04.23211565 -07 30 46.5746985   17.6 18.0 18.2   ~ 186 1
12 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3045 2
13 Mrk 231 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 1988 3
14 IC 860 LIN 13 15 03.51 +24 37 07.8   14.8       ~ 217 0
15 2MASX J13150638-5509225 Sy2 13 15 06.383 -55 09 22.60   17.3       ~ 147 0
16 Mrk 273 Sy2 13 44 42.1781 +55 53 12.819   15.68 14.91     ~ 913 3
17 Z 49-57 GiC 15 13 13.0927 +07 13 31.850   15.5       ~ 238 1
18 2MASX J15265942+3558372 LIN 15 26 59.442 +35 58 37.01   15.61       ~ 272 1
19 APG 220A PoG 15 34 57.22 +23 30 11.4           ~ 57 1
20 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2961 4
21 APG 220B PoG 15 34 57.28 +23 30 11.3           ~ 45 1
22 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1637 2
23 LEDA 60189 LIN 17 23 21.943 -00 17 00.96   15.1       ~ 424 0
24 NAME Super Antennae Sy2 19 31 21.4272801984 -72 39 21.442847832   17.39 16.37 14.65   ~ 302 2
25 6dFGS gJ204418.2-164017 LIN 20 44 18.186 -16 40 16.63   18.02   17.04   ~ 90 0
26 ESO 286-19 LIN 20 58 26.8183783008 -42 38 59.411838156   14.79 14.79 14.20   ~ 291 0
27 NAME South America H2G 22 51 49.307 -17 52 23.96   16.97       ~ 327 3
28 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2095 3

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