2024A&A...686A..48N


Query : 2024A&A...686A..48N

2024A&A...686A..48N - Astronomy and Astrophysics, volume 686A48 (2024/6-1)

CON-quest II. Spatially and spectrally resolved HCN/HCO+ line ratios in local luminous and ultraluminous infrared galaxies.

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

Abstract (from CDS):

Context. Nuclear regions of ultraluminous and luminous infrared galaxies (U/LIRGs) are powered by starbursts and/or active galactic nuclei (AGNs). These regions are often obscured by extremely high columns of gas and dust. Molecular lines in the submillimeter windows have the potential to determine the physical conditions of these compact obscured nuclei (CONs).
Aims. We aim to reveal the distributions of HCN and HCO+ emission in local U/LIRGs and investigate whether and how they are related to galaxy properties.
Methods. Using the Atacama Large Millimeter/submillimeter Array (ALMA), we have conducted sensitive observations of the HCN J = 3-2 and HCO+J = 3-2 lines toward 23 U/LIRGs in the local Universe (z < 0.07) with a spatial resolution of ∼0.3″ (∼50-400 pc).
Results. We detected both HCN and HCO+ in 21 galaxies, only HCN in one galaxy, and neither in one galaxy. The global HCN/HCO+ line ratios, averaged over scales of ∼0.5-4 kpc, range from 0.4 to 2.3, with an unweighted mean of 1.1. These line ratios appear to have no systematic trend with bolometric AGN luminosity or star formation rate. The line ratio varies with position and velocity within each galaxy, with an average interquartile range of 0.38 on a spaxel-by-spaxel basis. In eight out of ten galaxies known to have outflows and/or inflows, we found spatially and kinematically symmetric structures of high line ratios. These structures appear as a collimated bicone in two galaxies and as a thin spherical shell in six galaxies.
Conclusions. Non-LTE analysis suggests that the high HCN/HCO+ line ratio in outflows is predominantly influenced by the abundance ratio. Chemical model calculations indicate that the enhancement of HCN abundance in outflows is likely due to high-temperature chemistry triggered by shock heating. These results imply that the HCN/HCO+ line ratio can aid in identifying the outflow geometry when the shock velocity of the outflows is sufficiently high to heat the gas.

Abstract Copyright: © The Authors 2024

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

Simbad objects: 31

goto Full paper

goto View the references in ADS

Number of rows : 31
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 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
2 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
3 NGC 1097 LIN 02 46 19.059 -30 16 29.68 10.46 9.97 9.48 8.72 9.8 ~ 1448 3
4 Z 418-14 AG? 04 12 22.670 +05 32 49.13   15.50       ~ 170 0
5 IRAS 05189-2524 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 545 0
6 NGC 2369 Sy1 07 16 37.753 -62 20 37.51   13.23   11.56 12.3 ~ 137 0
7 NVSS J090412-362700 rG 09 04 12.70392 -36 27 01.1412           ~ 104 1
8 NGC 3110 Sy1 10 04 02.12400 -06 28 29.1250   13.4   13.3 12.5 ~ 191 2
9 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
10 IRAS 10565+2448 LIN 10 59 18.12811 +24 32 34.7357   15.7       ~ 302 0
11 MCG-06-26-013 EmG 11 53 11.722 -39 07 48.72   13.30   11.86   ~ 203 1
12 NGC 4194 rG 12 14 09.615 +54 31 35.93   13.79 13.30     ~ 467 2
13 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
14 2MASX J13150638-5509225 Sy2 13 15 06.33480 -55 09 22.7736   17.3       ~ 172 0
15 NGC 5135 Sy2 13 25 44.059 -29 50 01.24   12.58 13.35 11.53 12.2 ~ 500 1
16 ESO 173-15 AGN 13 27 23.774 -57 29 22.14   14.9   14.3 13.7 ~ 81 1
17 ESO 221-10 Sy2 13 50 56.924 -49 03 19.72   12.96 11.93 11.75 12.7 ~ 84 1
18 LEDA 89507 Sy2 14 40 59.0135478768 -37 04 31.938829896   17.72   16.48   ~ 131 1
19 NGC 5734 Sy2 14 45 09.0364267176 -20 52 13.484556696   13.75   12.08   ~ 89 1
20 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
21 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2
22 IRAS 17138-1017 Sy2 17 16 35.83992 -10 20 38.9832   17.43   14.59   ~ 143 0
23 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
24 2MFGC 14160 GiG 18 00 31.919 -04 00 53.36   17.62       ~ 69 0
25 IC 4734 AGN 18 38 25.6846404504 -57 29 25.078201116   14.21   12.71   ~ 95 0
26 LEDA 166649 AGN 19 56 35.7922773768 +11 19 05.126583432           ~ 65 0
27 LDN 1157 DNe 20 39 06.4 +68 02 13           ~ 606 0
28 MCG-07-43-014 AGN 21 04 11.162 -43 35 32.51   14.42   13.47 13.9 ~ 72 0
29 Mrk 1513 Sy1 21 32 27.8162556672 +10 08 19.252365396   14.92 14.64     ~ 651 0
30 IC 5179 Sy1 22 16 09.1191653256 -36 50 37.117603752   12.29 11.89 11.38   ~ 214 1
31 ESO 148-2 Sy2 23 15 46.76280 -59 03 15.6924   14.94 14.73 13.95   ~ 289 1

To bookmark this query, right click on this link: simbad:objects in 2024A&A...686A..48N and select 'bookmark this link' or equivalent in the popup menu