2021A&A...649A.105F


Query : 2021A&A...649A.105F

2021A&A...649A.105F - Astronomy and Astrophysics, volume 649A, 105-105 (2021/5-1)

CON-quest. Searching for the most obscured galaxy nuclei.

FALSTAD N., AALTO S., KONIG S., ONISHI K., MULLER S., GORSKI M., SATO M., STANLEY F., COMBES F., GONZALEZ-ALFONSO E., MANGUM J.G., EVANS A.S., BARCOS-MUNOZ L., PRIVON G.C., LINDEN S.T., DIAZ-SANTOS T., MARTIN S., SAKAMOTO K., HARADA N., FULLER G.A., GALLAGHER J.S., VAN DER WERF P.P., VITI S., GREVE T.R., GARCIA-BURILLO S., HENKEL C., IMANISHI M., IZUMI T., NISHIMURA Y., RICCI C. and MUHLE S.

Abstract (from CDS):


Context. Some luminous and ultraluminous infrared galaxies (LIRGs and ULIRGs) host extremely compact (r<100pc) and dusty nuclei. The high extinction associated with large column densities of gas and dust toward these objects render them hard to detect at many wavelengths. The intense infrared radiation arising from warm dust in these sources can provide a significant fraction of the bolometric luminosity of the galaxy and is prone to excite vibrational levels of molecules such as HCN. This results in emission from the rotational transitions of vibrationally excited HCN (HCN-vib); the brightest emission is found in compact obscured nuclei (CONs; ΣHCN–vib>1L/pc2 in the J=3-2 transition). However, there have been no systematic searches for CONs, and it is unknown how common they are.
Aims. We aim to establish how common CONs are in the local Universe (z<0.08), and whether their prevalence depends on the luminosity or other properties of the host galaxy.
Methods. We conducted an Atacama Large Millimeter/submillimeter Array survey of the rotational J=3-2 transition of HCN-vib in a volume-limited sample of 46 far-infrared luminous galaxies.
Results. Compact obscured nuclei are identified in 38–13^+18% of the ULIRGs, 21–6^+12% of the LIRGs, and 0–0^+9% of the lower luminosity galaxies. We find no dependence on the inclination of the host galaxy, but strong evidence of lower IRAS 25µm to 60µm flux density ratios (f25/f60) in CONs (with the exception of one galaxy, NGC 4418) compared to the rest of the sample. Furthermore, we find that CONs have stronger silicate features (s9.7µm), but similar polycyclic aromatic hydrocarbon equivalent widths (EQW6.2µm) compared to other galaxies. Along with signatures of molecular inflows seen in the far-infrared in most CONs, submillimeter observations also reveal compact, often collimated, outflows.
Conclusions. In the local Universe, CONs are primarily found in (U)LIRGs, in which they are remarkably common. As such systems are often highly disturbed, inclinations are difficult to estimate, and high-resolution continuum observations of the individual nuclei are required to determine if the CON phenomenon is related to the inclinations of the nuclear disks. Further studies of the in- and outflow properties of CONs should also be conducted to investigate how these are connected to each other and to the CON phenomenon. The lower f25/f60 ratios in CONs as well as the results for the mid-infrared diagnostics investigated (EQW6.2µm and s9.7µm) are consistent with the notion that large dust columns gradually shift the radiation from the hot nucleus to longer wavelengths, making the mid- and far-infrared "photospheres" significantly cooler than the interior regions. Finally, to assess the importance of CONs in the context of galaxy evolution, it is necessary to extend this study to higher redshifts where (U)LIRGs are more common.

Abstract Copyright: © ESO 2021

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

Simbad objects: 55

goto Full paper

goto View the references in ADS

Number of rows : 55
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 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3336 2
2 NGC 613 AGN 01 34 18.235 -29 25 06.56   10.77 12.71 9.50 10.6 ~ 409 3
3 NGC 660 Sy2 01 43 02.350 +13 38 44.45   12.02 11.16     ~ 556 2
4 NGC 713 EmG 01 55 21.5313772488 -09 05 01.667450616   15   13.94   ~ 22 0
5 NGC 1055 GiP 02 41 45.233 +00 26 35.45 11.59 11.40 10.59 10.5 10.7 ~ 283 2
6 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4601 2
7 UGC 2982 AG? 04 12 22.670 +05 32 49.13   15.50       ~ 159 0
8 NGC 1559 GiG 04 17 35.7508602240 -62 47 01.251567384   11.19 10.45 10.11 10.4 ~ 282 1
9 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 667 0
10 NGC 1792 Sy1 05 05 14.4036930408 -37 58 50.064531168   10.68 10.18 9.53 10.4 ~ 234 1
11 NGC 1808 Sy2 05 07 42.343 -37 30 46.98 11.05 10.80 9.94 9.36 10.2 ~ 721 3
12 LEDA 89499 Sy2 06 02 54.066 -71 03 10.48   15.6       ~ 94 1
13 NGC 2369 Sy1 07 16 37.753 -62 20 37.51   13.23   11.56 12.3 ~ 130 0
14 2MASX J09041268-3627007 G 09 04 12.689 -36 27 00.76           ~ 85 0
15 NGC 3110 Sy1 10 04 02.0 -06 28 29   13.4   13.3 12.5 ~ 174 3
16 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 848 2
17 M 66 GiP 11 20 15.0 +12 59 29 9.85 9.65 8.92     ~ 1386 4
18 NGC 3628 GiP 11 20 17.018 +13 35 22.16   10.42 9.48 9.22   ~ 827 3
19 NGC 3810 GiG 11 40 58.7615811624 +11 28 15.808680696   11.4       ~ 335 2
20 ESO 320-30 EmG 11 53 11.722 -39 07 48.72   13.30   11.86   ~ 186 1
21 LEDA 39024 LIN 12 13 46.107 +02 48 41.50           ~ 354 1
22 M 99 H2G 12 18 49.625 +14 24 59.36 10.45 10.44 9.87     ~ 918 2
23 M 61 Sy2 12 21 54.9282582888 +04 28 25.597367184 10.07 10.18 9.65     ~ 996 2
24 NGC 4355 Sy2 12 26 54.6206739120 -00 52 39.421212996   14.21 13.37     ~ 491 2
25 M 88 Sy2 12 31 59.1525062448 +14 25 13.148971824   14.33 13.18     ~ 804 1
26 NGC 4527 GiP 12 34 08.4 +02 39 15   12.4       ~ 532 2
27 NGC 4536 GiP 12 34 27.1 +02 11 18 11.14 11.16 10.55 17.393   ~ 852 3
28 NGC 4568 GiP 12 36 34.292 +11 14 19.07   12.11 11.19     ~ 380 2
29 NGC 4654 GiP 12 43 56.638 +13 07 34.86   11.8       ~ 567 1
30 NGC 4666 EmG 12 45 08.676 -00 27 42.88   11.7   11.5 10.7 ~ 387 1
31 Mrk 231 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 1987 3
32 IC 860 LIN 13 15 03.51 +24 37 07.8   14.8       ~ 217 0
33 2MASX J13150638-5509225 Sy2 13 15 06.383 -55 09 22.60   17.3       ~ 147 0
34 NGC 5135 Sy2 13 25 44.059 -29 50 01.24   12.58 13.35 11.53 12.2 ~ 474 1
35 ESO 173-15 AG? 13 27 23.774 -57 29 22.14   14.9   14.3 13.7 ~ 75 1
36 NGC 5248 GiG 13 37 32.0145074088 +08 53 06.496982448   11.4       ~ 508 0
37 ESO 221-10 Sy2 13 50 56.924 -49 03 19.72   12.96 11.93 11.75 12.7 ~ 77 0
38 NGC 5643 Sy2 14 32 40.778 -44 10 28.60   11.03 13.60 9.92 10.6 ~ 572 0
39 LEDA 52270 Sy1 14 37 38.2867288488 -15 00 24.087592692   16.58 16.40     ~ 276 1
40 LEDA 89507 Sy2 14 40 59.0135478768 -37 04 31.938829896   17.72   16.48   ~ 118 0
41 NGC 5734 Sy2 14 45 09.0364267176 -20 52 13.484556696   13.75   12.08   ~ 81 1
42 Z 49-57 GiC 15 13 13.0927 +07 13 31.850   15.5       ~ 238 1
43 APG 220A PoG 15 34 57.22 +23 30 11.4           ~ 57 1
44 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2961 4
45 APG 220B PoG 15 34 57.28 +23 30 11.3           ~ 45 1
46 IRAS 17138-1017 Sy2 17 16 35.83992 -10 20 38.9832   17.43   14.59   ~ 131 0
47 LEDA 60189 LIN 17 23 21.943 -00 17 00.96   15.1       ~ 424 0
48 2MFGC 14160 GiG 18 00 31.919 -04 00 53.36   17.62       ~ 64 0
49 IC 4687 AGN 18 13 39.829 -57 43 31.25   14.35 14.3 12.78   ~ 136 1
50 IC 4734 GiG 18 38 25.6846404504 -57 29 25.078201116   14.21   12.71   ~ 85 0
51 ESO 286-35 GiG 21 04 11.162 -43 35 32.51   14.42   13.47 13.9 ~ 61 0
52 NGC 7130 Sy2 21 48 19.5412287192 -34 57 04.492024884   12.86 13.87 11.57   ~ 450 0
53 IC 5179 Sy1 22 16 09.1191653256 -36 50 37.117603752   12.29 11.89 11.38   ~ 204 1
54 NAME South America H2G 22 51 49.307 -17 52 23.96   16.97       ~ 327 3
55 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2095 3

To bookmark this query, right click on this link: simbad:objects in 2021A&A...649A.105F and select 'bookmark this link' or equivalent in the popup menu