2023A&A...673A..13M


Query : 2023A&A...673A..13M

2023A&A...673A..13M - Astronomy and Astrophysics, volume 673A13 (2023/5-1)

A sensitive APEX and ALMA CO(1-0), CO(2-1), CO(3-2), and [CI](1-0) spectral survey of 40 local (ultra-)luminous infrared galaxies.

MONTOYA ARROYAVE I., CICONE C., MAKROLEIVADITI E., WEISS A., LUNDGREN A., SEVERGNINI P., DE BREUCK C., BAUMSCHLAGER B., SCHIMEK A., SHEN S. and ARAVENA M.

Abstract (from CDS):

We present a high sensitivity, ground-based spectral line survey of low-J carbon monoxide (CO(Jup → Jup - 1) with Jup = 1, 2, 3) and neutral carbon [CI] 3P1-3P0 ([CI](1-0)) in 36 local ultra-luminous infrared galaxies (ULIRGs) and 4 additional LIRGs, all of which have previous Herschel OH 119 μm observations. The study is based on new single-dish observations conducted with the Atacama Pathfinder Experiment (APEX) and complemented with archival APEX and Atacama Large Millimeter Array (ALMA and ACA) data. Our methods are optimized for a multi-tracer study of the total molecular line emission from these ULIRGs, including any extended low-surface-brightness components. We find a tight correlation between the CO and [CI] line luminosities, which suggests that the emission from CO(1-0) (and CO(2-1)) arises from similar regions as the [CI](1-0), at least when averaged over galactic scales. By using [CI] to compute molecular gas masses, we estimate a median CO-to-H2 conversion factor of ⟨αCO⟩ = 1.7 ± 0.5 M⊙ (K km s–1pc2)–1 for ULIRGs. We derive median galaxy-integrated CO line ratios of $ \langle r_{21} \rangle = L^\prime_{{\rm CO(2-1)}}/L^\prime_{{\rm CO(1-0)}} = 1.09 $ , $ \langle r_{31} \rangle = L^\prime_{{\rm CO(3-2)}}/L^\prime_{{\rm CO(1-0)}} = 0.76 $ , and $ \langle r_{32} \rangle = L^\prime_{{\rm CO(3-2)}}/L^\prime_{{\rm CO(2-1)}} = 0.76 $ , significantly higher than normal star-forming galaxies, confirming the exceptional molecular gas properties of ULIRGs. We find that the r21 and r32 ratios are poor tracers of CO excitation in ULIRGs, while r31 shows a positive trend with LIR and star formation rates and a negative trend with the H2 gas depletion timescales (τdep). Our investigation of CO line ratios as a function of gas kinematics shows no clear trends, except for a positive relation between r21 and σv, which can be explained by CO opacity effects. These ULIRGs are also characterized by high $ L^\prime_{\rm [CI](1-0)}/L^\prime_{\rm CO(1-0)} $ ratios, with a measured median value of ⟨rCICO⟩ = 0.18, higher than values from previous interferometric studies that were affected by missing [CI] line flux. The rCICO values do not show a significant correlation with any of the galaxy properties investigated, including OH outflow velocities and equivalent widths. We find that the widths of [CI](1-0) lines are ∼10% smaller than those of CO lines, and that this discrepancy becomes more significant in ULIRGs with broad lines (σv > 150 km s–1) and when considering the high-v wings of the lines. This suggests that the low optical depth of [CI] can challenge its detection in diffuse, low-surface-brightness outflows and, therefore, its use as a tracer of CO-dark H2 gas in these components. Finally, we find that higher LAGN are associated with longer τdep, consistent with the hypothesis that active galactic nucleus feedback may reduce the efficiency of star formation. Our study highlights the need for sensitive single-dish multi-tracer H2 surveys of ULIRGs that are able to recover the flux that is missed by interferometers, especially in the high-frequency lines such as [CI]. The Atacama Large Aperture Submillimeter Telescope (AtLAST) will be transformational for this field.

Abstract Copyright: © The Authors 2023

Journal keyword(s): galaxies: evolution - submillimeter: galaxies - galaxies: active - galaxies: starburst - galaxies: ISM - galaxies: interactions

Simbad objects: 51

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Number of rows : 51
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 2MASX J00212652-0839261 LIN 00 21 26.5135306416 -08 39 25.967117268   18.37       ~ 124 1
2 LEDA 165307 AGN 00 42 15.51192 -12 56 03.3108   19.45       ~ 86 0
3 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
4 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
5 IRAS 01003-2238 Sy2 01 02 49.9920152640 -22 21 57.262136544   18.62 18.9 17.83   ~ 192 0
6 Mrk 1014 Sy1 01 59 50.2534701768 +00 23 40.864244784   16.08 15.87     ~ 606 0
7 NGC 891 H2G 02 22 32.907 +42 20 53.95 11.08 10.81 9.93 7.86   ~ 1741 2
8 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
9 IRAS 03521+0028 AGN 03 54 42.14640 +00 37 03.3280           ~ 104 0
10 LEDA 2816449 Sy2 05 04 36.53952 -19 37 03.1332           ~ 39 1
11 IRAS 05189-2524 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 545 0
12 LEDA 89499 Sy2 06 02 53.95560 -71 03 10.1448   15.6       ~ 107 1
13 LEDA 89500 Sy2 06 21 01.17192 -63 17 23.6616   16.70   15.27   ~ 79 1
14 2MASS J07273756-0254540 AGN 07 27 37.5366009312 -02 54 54.264024396           ~ 69 0
15 2MASX J08332058-2509332 Sy1 08 33 20.59608 -25 09 33.8220   16.4       ~ 44 0
16 NVSS J090412-362700 rG 09 04 12.70392 -36 27 01.1412           ~ 104 1
17 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
18 NGC 3110 Sy1 10 04 02.12400 -06 28 29.1250   13.4   13.3 12.5 ~ 191 2
19 IRAS 10378+1109 Sy1 10 40 29.1640944744 +10 53 18.202070076   17.79 17.18     ~ 115 1
20 LEDA 125693 LIN 11 12 03.37008 -02 54 22.7232   17.45 17.40     ~ 113 1
21 Mrk 1298 Sy1 11 29 16.7288400936 -04 24 07.246460520   14.97 14.61     ~ 224 1
22 LEDA 90164 Sy2 12 09 45.1187842872 -05 01 13.431047484   17.52 17.8 16.56   ~ 114 1
23 IRAS 12112+0305 PaG 12 13 45.98880 +02 48 39.9600           ~ 373 0
24 [CGM90] IRAS 12112+0305 NE rG 12 13 46.10735 +02 48 41.4959           ~ 369 0
25 NGC 4355 Sy2 12 26 54.6206739120 -00 52 39.421212996   14.21 13.37     ~ 527 2
26 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
27 2MASX J13150638-5509225 Sy2 13 15 06.33480 -55 09 22.7736   17.3       ~ 172 0
28 IRAS 13305-1739 Sy1 13 33 16.5631735944 -17 55 10.612057080   20.0 18.6     ~ 47 1
29 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
30 PKS 1345+12 Sy2 13 47 33.36161873 +12 17 24.2398927   19.28 18.44 15.718   ~ 652 2
31 LEDA 52270 Sy1 14 37 38.2867288488 -15 00 24.087592692   16.58 16.40     ~ 300 2
32 LEDA 89507 Sy2 14 40 59.0135478768 -37 04 31.938829896   17.72   16.48   ~ 131 1
33 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
34 LEDA 90222 Sy1 15 48 56.8020209304 -04 59 33.598051584   16.4 16.40 16.85   ~ 106 0
35 LEDA 90237 LIN 16 11 40.4280459768 -01 47 06.566246232   16.6       ~ 95 0
36 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2
37 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
38 NAME Super Antennae Sy2 19 31 21.4272801984 -72 39 21.442847832   17.39 16.37 14.65   ~ 318 3
39 NVSS J193222-040000 rG 19 32 22.2962473608 -04 00 01.797249204   18.85   17.04   ~ 122 0
40 LEDA 166649 AGN 19 56 35.7922773768 +11 19 05.126583432           ~ 65 0
41 LEDA 90352 LIN 20 11 23.86872 -02 59 50.7588   17.80   16.41   ~ 78 0
42 [VV2000] J201329.8-414735 QSO 20 13 29.55552 -41 47 35.0592   17.0       ~ 141 2
43 6dFGS gJ204418.2-164017 LIN 20 44 18.16392 -16 40 16.8132   18.02   17.04   ~ 100 0
44 ESO 286-19 LIN 20 58 26.8183783008 -42 38 59.411838156   14.79 14.79 14.20   ~ 318 0
45 Mrk 1513 Sy1 21 32 27.8162556672 +10 08 19.252365396   14.92 14.64     ~ 651 0
46 NAME South America rG 22 51 49.27872 -17 52 24.0600   16.97       ~ 348 3
47 IRAS 23060+0505 Sy1 23 08 33.9537309816 +05 21 29.751752412           ~ 160 0
48 ESO 148-2 Sy2 23 15 46.76280 -59 03 15.6924   14.94 14.73 13.95   ~ 289 1
49 LEDA 90424 LIN 23 26 03.6867143064 -69 10 18.422274828   16.6       ~ 60 0
50 LEDA 90425 rG 23 28 06.0899186859 -53 58 30.679199450   17.19   16.10   ~ 49 1
51 87GB 233856.4+030039 LIN 23 41 30.3076816728 +03 17 26.572938864     20.0     ~ 55 1

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