2026A&A...707A.144S


Query : 2026A&A...707A.144S

2026A&A...707A.144S - Astronomy and Astrophysics, volume 707A144 (2026/3-1)

Spatially resolved star formation relations in local luminous infrared galaxies along the complete merger sequence.

SANCHEZ-GARCIA M., DIAZ-SANTOS T., BARCOS-MUNOZ L., EVANS A.S., SONG Y., PEREIRA-SANTAELLA M., GARCIA-BURILLO S., LINDEN S.T., RICCI C., LENKIC L., ZANELLA A., ARMUS L., EIBENSTEINER C., TENG Y.-H., SARAVIA A., BUITEN V.A., PRIVON G.C., TORRES-ALBA N., SAITO T., LARSON K.L., BIANCHIN M., MEDLING A.M., LAI T., DONNELLY G.P., CHARMANDARIS V., BOHN T., LOFARO C.M. and MEZA G.

Abstract (from CDS):

We investigated the properties of the interstellar medium (ISM) at giant molecular cloud (GMC) scales (∼100 pc) in a sample of 27 nearby luminous infrared galaxies (LIRGs) spanning all interacting stages along the merger sequence, i.e. from isolated systems to late-stage mergers. In particular, we study the relations between star-formation (SF) and molecular gas surface density as a function of the interaction stage by (1) defining beam-sized (unresolved, line-of-sight) regions and (2) identifying actual gas clumps and physical structures within the galaxies. In total, we identify more than 4000 beam-sized CO-emitting regions defined on scales of ∼100 pc and more than 1000 molecular gas clumps in the sample. To map the distribution of molecular gas we used the Atacama Large Millimeter/submillimeter Array (ALMA) to observe the J = 2-1 CO transition, and to map the distribution of star formation we used the Hubble Space Telescope (HST) observations of the Paα or Paβ hydrogen recombination lines. We derived spatially resolved Kennicutt-Schmidt (KS) relations for each LIRG in the sample. When using beam-sized regions, we find that 67% of galaxies follow a single relation between ΣSFR and ΣH2. However, in the remaining galaxies, the relation splits into two branches - one characterised by higher ΣSFR and ΣH2, the other by lower value - indicating the presence of a duality in this relation. In contrast, when using physical gas clumps, the duality disappears and all galaxies show a single trend. These results provide two complementary perspectives when studying the star formation process. The first maximises the number statistics (beam-sized regions), and the second focuses on actual structures associated with gas clumps in which the measured sizes have a physical meaning. We also studied other ISM and clump properties as a function of the merger stage of the LIRG systems. We find that isolated galaxies and systems in early stages of interaction exhibit smaller amounts of gas and lower star formation rates (SFRs). As the merger progresses, however, the amount of gas in the central kiloparsecs of the galaxy undergoing the merger increases, along with the SFR, and the slope of the KS relation becomes steeper, indicating an increase in the SF efficiency of the molecular gas clumps. Clumps in late-stage mergers are predominantly located at small distances from the nucleus, confirming that most of the activity is concentrated in the central regions. Interestingly, the relation between the star formation efficiency and the boundedness parameter (which measures the effects of gravity against velocity dispersion) evolves from being roughly flat in the early stages of the merger to becoming positive in the final phases, indicating that clump self-gravity only starts to regulate the star formation process between the early and mid merger stages.

Abstract Copyright: © The Authors 2026

Journal keyword(s): ISM: clouds - galaxies: interactions - galaxies: ISM - galaxies: star formation

VizieR on-line data: <Available at CDS (J/A+A/707/A144): table6.dat>

Status at CDS : Tables of objects will be appraised for possible ingestion in SIMBAD.

Simbad objects: 27

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Number of rows : 27
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 MCG-02-01-052 EmG 00 18 50.152 -10 21 41.49   13 13.60 14.13   ~ 68 3
2 MCG-02-01-051 Sy2 00 18 50.898 -10 22 36.49   14.81 14.33     ~ 154 3
3 M 74 G 01 36 41.7451236624 +15 47 01.107512304 10.52 10.00 9.46 9.16   ~ 1934 1
4 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 697 1
5 NGC 2369 Sy1 07 16 37.753 -62 20 37.51   13.23   11.56 12.3 ~ 137 0
6 LEDA 90088 AGN 08 37 01.827 -49 54 30.27           ~ 67 0
7 NGC 3110 Sy1 10 04 02.12400 -06 28 29.1250   13.4   13.3 12.5 ~ 191 2
8 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
9 MCG-06-26-013 EmG 11 53 11.722 -39 07 48.72   13.30   11.86   ~ 203 1
10 MCG-02-33-098 AG? 13 02 19.5 -15 46 05   14       ~ 96 0
11 2MASX J13150638-5509225 Sy2 13 15 06.33480 -55 09 22.7736   17.3       ~ 172 0
12 IC 883 SBG 13 20 35.37960 +34 08 21.8400   14.8       ~ 421 1
13 NGC 5135 Sy2 13 25 44.059 -29 50 01.24   12.58 13.35 11.53 12.2 ~ 500 1
14 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
15 NGC 5257 H2G 13 39 52.92781 +00 50 24.0903   13.7 12.99     ~ 208 0
16 APG 240 PaG 13 39 55.06 +00 50 06.4   12.6       ~ 158 0
17 NGC 5258 GiP 13 39 57.6768310848 +00 49 51.009668076   13.8 12.83     ~ 186 0
18 NGC 5331 GiP 13 52 16.289 +02 06 04.18           ~ 97 0
19 IC 4518 Sy2 14 57 45.6 -43 07 58   14.5       ~ 81 0
20 ESO 99-4 G 15 24 58.217 -63 07 34.43   16.4       ~ 51 0
21 IRAS 16164-0746 Sy1 16 19 11.792 -07 54 02.61   15.49       ~ 88 1
22 IRAS 17138-1017 Sy2 17 16 35.83992 -10 20 38.9832   17.43   14.59   ~ 143 0
23 IC 4687 AGN 18 13 39.829 -57 43 31.25   14.35 14.3 12.78   ~ 143 2
24 IC 4734 AGN 18 38 25.6846404504 -57 29 25.078201116   14.21   12.71   ~ 95 0
25 NGC 7130 Sy2 21 48 19.5412287192 -34 57 04.492024884   12.86 13.87 11.57   ~ 483 1
26 IC 5179 Sy1 22 16 09.1191653256 -36 50 37.117603752   12.29 11.89 11.38   ~ 214 1
27 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2253 3

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