2025A&A...696A.228G


Query : 2025A&A...696A.228G

2025A&A...696A.228G - Astronomy and Astrophysics, volume 696A228 (2025/4-1)

Clump formation in ram-pressure stripped galaxies: Evidence from mass function.

GIUNCHI E., SCARLATA C., WERLE A., POGGIANTI B.M., MORETTI A., GULLIEUSZIK M., VULCANI B., IGNESTI A., MARASCO A., ZANELLA A. and WOLTER A.

Abstract (from CDS):

Context. The mass function (MF) of young stellar clumps (age ≲ 200 Myr) is an indicator of the mechanism driving the collapse of the interstellar medium (ISM) into the giant molecular clouds. Typically, the MF of clumps in main-sequence galaxies is described by a power law (dN/dM* ∝ M*^-α^) with slope α = 2, hinting that the collapse is driven by turbulence.
Aims. To understand whether the local environment affects star formation, we modelled the clump MF of six cluster galaxies, from the GASP survey, undergoing strong ram-pressure stripping (RPS). This phenomenon, exerted by the hot and high-pressure intracluster medium (ICM), has produced long tails of stripped ISM, where clumps form far away from the galactic disk and are surrounded by the ICM itself.
Methods. Clumps were selected from HST-UVIS/WFC3 images, covering from near-UV to red-optical bands and including Hα emission-line maps. The catalogue comprises 398 Hα clumps (188 in tails, 210 in the disk outskirts known as the extraplanar region) and 1270 UV clumps (593 in tails, 677 extraplanar). Using mock images, we quantified the mass completeness and bias of our sample. Taking these two effects into account, we adopted a Bayesian approach to fit the clump mass catalogue to a suitable MF.
Results. The resulting MFs are steeper than the expected value of 2. In the tails the Hα clumps have slope α = 2.31 ± 0.12, while the UV slope is larger (2.60 ± 0.09), in agreement with ageing effects. Similar results are found in the extraplanar region, with Hα slope $ \alpha=2.45^{+0.20}_{-0.16} $ and UV slope $ \alpha=2.63^{+0.20}_{-0.18} $, even though in this case they are consistent within the uncertainties.
Conclusions. We suggest that the steepening results from the higher-than-usual turbulent environment, arising from the interaction between the ISM and the ICM. As shown by recent works, this process can favour the fragmentation of the largest ISM clouds, inhibiting the formation of very massive clumps.

Abstract Copyright: © The Authors 2025

Journal keyword(s): galaxies: clusters: general - galaxies: evolution - galaxies: peculiar - galaxies: star formation - galaxies: structure

Simbad objects: 15

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Number of rows : 15
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 Ka 364 SyG 00 41 30.2986763472 -09 15 45.892857024   16.2 14.46 14.32   ~ 86 0
2 ACO 85 ClG 00 41 36.21 -09 19 30.4           ~ 974 0
3 Z 8-77 Sy2 10 13 46.8173594520 -00 54 51.236467848   18.25 17.58 15.014   ~ 78 0
4 ACO 957 ClG 10 14 02.35 -00 53 30.0           ~ 225 2
5 ACO 1668 ClG 13 04 00.60 +19 17 09.6           ~ 132 0
6 IC 4141 LIN 13 04 07.7273080968 +19 12 38.359601172   17       ~ 38 0
7 Cl Moffat 1 OpC 16 01 38.5 -54 08 56           ~ 26 0
8 ESO 137-1 AG? 16 13 27.305 -60 45 50.59   14.84   13.87   ~ 132 0
9 Cl Moffat 2 OpC 17 14 27.65 -39 45 59.9           ~ 7 0
10 ACO 3716 ClG 20 51 16.7 -52 41 43           ~ 123 1
11 2MASX J20511757-5249221 GiC 20 51 17.5759828848 -52 49 22.002814596   15   15.77   ~ 25 0
12 2MASX J21134738+0228347 AGN 21 13 47.4035338272 +02 28 34.520551932           ~ 40 0
13 Z 375-15 BiC 21 13 55.918 +02 33 55.39   15.1       ~ 67 1
14 IC 5337 AGN 23 36 25.0391944872 +21 09 02.907865116   15.4       ~ 81 0
15 ACO 2626 ClG 23 36 31.0 +21 09 36           ~ 265 0

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