2021A&A...646A..25Z


Query : 2021A&A...646A..25Z

2021A&A...646A..25Z - Astronomy and Astrophysics, volume 646A25-25 (2021/2-1)

H II regions and high-mass starless clump candidates. II. Fragmentation and induced star formation at ∼0.025 pc scale: an ALMA continuum study.

ZHANG S., ZAVAGNO A., LOPEZ-SEPULCRE A., LIU H., LOUVET F., FIGUEIRA M., RUSSEIL D., WU Y., YUAN J. and PILLAI T.G.S.

Abstract (from CDS):


Context. The ionization feedback from HII regions modifies the properties of high-mass starless clumps (HMSCs, of several hundred to a few thousand solar masses with a typical size of 0.1-1pc), such as dust temperature and turbulence, on the clump scale. The question of whether the presence of HII regions modifies the core-scale (∼0.025pc) fragmentation and star formation in HMSCs remains to be explored.
Aims. We aim to investigate the difference of 0.025pc-scale fragmentation between candidate HMSCs that are strongly impacted by HII regions and less disturbed ones. We also search for evidence of mass shaping and induced star formation in the impacted candidate HMSCs.
Methods. Using the ALMA 1.3 mm continuum, with a typical angular resolution of 1.3'', we imaged eight candidate HMSCs, including four impacted by HII regions and another four situated in the quiet environment. The less-impacted candidate HMSCs are selected on the basis of their similar mass and distance compared to the impacted ones to avoid any possible bias linked to these parameters. We carried out a comparison between the two types of candidate HMSCs. We used multi-wavelength data to analyze the interaction between HII regions and the impacted candidate HMSCs.
Results. A total of 51 cores were detected in eight clumps, with three to nine cores for each clump. Within our limited sample, we did not find a clear difference in the ∼0.025pc-scale fragmentation between impacted and non-impacted candidate HMSCs, even though HII regions seem to affect the spatial distribution of the fragmented cores. Both types of candidate HMSCs present a thermal fragmentation with two-level hierarchical features at the clump thermal Jeans length λJ,clumpth and 0.3λJ,clumpth. The ALMA emission morphology of the impacted candidate HMSCs AGAL010.214-00.306 and AGAL018.931-00.029 sheds light on the capacities of HII regions to shape gas and dust in their surroundings and possibly to trigger star formation at ∼0.025pc-scale in candidate HMSCs.
Conclusions. The fragmentation at ∼0.025pc scale for both types of candidate HMSCs is likely to be thermal-dominant, meanwhile HII regions probably have the capacity to assist in the formation of dense structures in the impacted candidate HMSCs. Future ALMA imaging surveys covering a large number of impacted candidate HMSCs with high turbulence levels are needed to confirm the trend of fragmentation indicated in this study.

Abstract Copyright: © S. Zhang et al. 2021

Journal keyword(s): stars: formation - stars: massive - HII regions - ISM: structure - submillimeter: ISM - techniques: interferometric

CDS comments: G022.495-00.261 not in SIMBAD.

Simbad objects: 31

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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 SH 2-201 HII 03 03 17.9 +60 27 52           ~ 118 0
2 NAME OMC-1 MoC 05 35 14 -05 22.4           ~ 1249 2
3 PMN J1603-4904 BLL 16 03 50.68456556 -49 04 05.5056817   20.67       ~ 89 1
4 AGAL G333.016-00.751 Y*O 16 21 56 -50 53.8           ~ 14 0
5 ICRF J165016.6-504448 QSO 16 50 16.62710806 -50 44 48.2106956   20.95       ~ 89 2
6 AGAL G341.039-00.114 MoC 16 51 14 -44 31.4           ~ 20 0
7 SH 2-3 HII 17 12.4 -38 28           ~ 234 1
8 NGC 6334 HII 17 20 53 -36 07.9           ~ 740 0
9 QSO B1730-130 Bla 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1198 1
10 AGAL G009.951-00.366 smm 18 09 01 -20 30.7           ~ 10 0
11 AGAL G010.214-00.306 cor 18 09 20 -20 15.1           ~ 27 0
12 [ABB2014] WISE G010.227-00.303 bub 18 09 22.2 -20 14 11           ~ 8 2
13 [WZT2014] P6-SMA 1 smm 18 10 07.80 -19 29 01.2           ~ 12 0
14 W 31 SFR 18 10 28.6 -19 55 51           ~ 280 0
15 [CBH2011b] G11.92-0.61 MM2 mm 18 13 57.860 -18 54 14.04           ~ 18 0
16 BD-15 4928 ** 18 20 13.71600 -15 39 53.3160 10.21 11.08 10.44     OB 9 0
17 AGAL G015.503-00.419 Y*O 18 20 22.836 -15 39 24.95           ~ 13 0
18 AGAL G018.931-00.029 Y*O 18 25 36 -12 26.9           ~ 13 0
19 AGAL G018.801-00.297 Y*O 18 26 19 -12 41.3           ~ 12 0
20 NVSS J183211-203947 BLL 18 32 11.0455806144 -20 39 48.210054948   18.56 20.2     ~ 75 1
21 PMN J1832-1035 rG 18 32 20.83647 -10 35 11.1968           ~ 107 1
22 AGAL G022.531-00.192 smm 18 32 59.520 -09 19 58.46           ~ 13 0
23 QSO B1830-211 Bla 18 33 39.9399138048 -21 03 39.368838780     18.70 21   ~ 724 1
24 [KTC2017] C9A cor 18 42 52.02 -03 59 46.8           ~ 6 0
25 AGAL G029.556+00.186 cor 18 44 37 -02 55.0           ~ 29 0
26 [L89b] 28.823-00.226 bub 18 44 44.3 -03 45 34           ~ 80 0
27 [MNL2018] 6 cor 18 47 46.160 -01 54 33.30           ~ 12 0
28 QSO J1851+005 QSO 18 51 46.72295 +00 35 32.3649           ~ 138 1
29 [BMC2010] CygX-N53 MM2 mm 20 39 03.22 +42 25 51.2           ~ 17 0
30 GAL 333.0-00.5 ? ~ ~           ~ 2 0
31 NAME Carina Region reg ~ ~           ~ 192 0

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