2022A&A...658A.102O


Query : 2022A&A...658A.102O

2022A&A...658A.102O - Astronomy and Astrophysics, volume 658A102-102 (2022/2-1)

Unveiling the substructure of the massive clump AGAL G035.1330-00.7450.

ORTEGA M.E., MARINELLI A., ISEQUILLA N.L. and PARON S.

Abstract (from CDS):


Context. It is known that high-mass stars form as the result of the fragmentation of massive molecular clumps. However, it is not clear whether this fragmentation gives rise to cores that are massive enough to directly form high-mass stars, or if leads to cores of low and intermediate masses that generate high-mass stars by acquiring material from their environment.
Aims. Detailed studies of massive clumps at the early stage of star formation are needed to collect observational evidence that sheds light on the fragmentation processes from clump to core scales. The infrared-quiet massive clump AGAL G035.1330-00.7450 (AGAL35) located at a distance of 2.1 kpc is a promising object for studying the fragmentation and the star formation activity at early stages.
Methods. Using millimeter observations of continuum and molecular lines obtained from the Atacama Large Millimeter Array database at Bands 6 and 7, we studied the substructure of the source AGAL35. The angular resolution of the data at Band 7 is about 0.7", which allowed us to resolve structures of about 0.007 pc (∼1500 au).
Results. The continuum emission at Bands 6 and 7 shows that AGAL35 harbors four dust cores, labeled C1 to C4, with masses lower than 3 M☉. Cores C3 and C4 exhibit well-collimated, young, and low-mass molecular outflows related to molecular hydrogen emission-line objects that were previously detected. Cores C1 and C2 present CH3CN J = 13-12 emission, from which we derive rotational temperatures of about 180 and 100 K, respectively. These temperatures allow us to estimate masses of about 1.4 and 0.9 M☉ for C1 and C2, respectively, which are about an order of magnitude lower than those estimated in previous works and agree with the Jeans mass of this clump. In particular, the moment 1 map of CH3CN emission suggests the presence of a rotating disk towards C1, which is confirmed by the CH3OH and CH3OCHO (20-19) emissions. On the other hand, the CN N = 2-1 emission shows a clumpy and filamentary structure that seems to connect all the cores. These filaments might be tracing the remnant gas of the fragmentation processes taking place within the massive clump AGAL35 or the gas that is being transported toward the cores, which would imply a competitive accretion scenario.
Conclusions. The massive clump AGAL35 harbors four low- to intermediate-mass cores with masses lower than 3 M☉, which is about an order of magnitude smaller than the masses estimated in previous works. This study shows that in addition to the importance of high-resolution and sensitivity observations for a complete detection of all fragments, it is very important to accurately determine the temperature of these cores for a correct mass estimation. Finally, although no high-mass cores were detected toward AGAL35, the filamentary structure connecting all the cores means that high-mass stars might form through the competitive accretion mechanism.

Abstract Copyright: © ESO 2022

Journal keyword(s): stars: formation - ISM: molecules - ISM: jets and outflows

Nomenclature: Figs 2-5, Table 2: [OMI2022] AGAL G035.1330-00.7450 CN (Nos C1-C4).

CDS comments: Paragraph 4.2, fig.4 molecular outflows OC3 and OC4 not in SIMBAD.

Simbad objects: 22

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Number of rows : 22
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 MSXDC G034.43+00.24 MoC 18 53 18.9 +01 26 39           ~ 122 0
2 MSXDC G035.39-00.33 MoC 18 57 09.0 +02 07 46           ~ 132 0
3 [MCM2005b] 14 Cl* 18 58 05 +01 36.6           ~ 7 0
4 [FI2011] MHO 2423 A out 18 58 05.9 +01 37 20           ~ 2 0
5 AGAL G035.132-00.744 smm 18 58 06 +01 37.1           ~ 20 0
6 [OMI2022] AGAL G035.1330-00.7450 C1 cor 18 58 06.10 +01 37 07.1           ~ 1 0
7 [CBW2017] G035.1330-00.7450-MM1 cor 18 58 06.19 +01 37 07.5           ~ 2 0
8 [OMI2022] AGAL G035.1330-00.7450 C2 cor 18 58 06.30 +01 37 07.4           ~ 1 0
9 EGO G035.13-0.74 of? 18 58 06.4 +01 37 01           ~ 13 0
10 [FI2011] MHO 2424 A out 18 58 06.5 +01 36 52           ~ 2 0
11 [CBW2017] G035.1330-00.7450-MM2 cor 18 58 06.58 +01 37 02.5           ~ 2 0
12 [OMI2022] AGAL G035.1330-00.7450 C4 cor 18 58 06.60 +01 37 02.2           ~ 1 0
13 [OMI2022] AGAL G035.1330-00.7450 C3 cor 18 58 06.60 +01 37 05.0           ~ 1 0
14 [ABB2014] WISE G035.126-00.755 bub 18 58 06.6 +01 36 21           ~ 5 0
15 [FI2011] MHO 2426 A out 18 58 06.7 +01 37 15           ~ 2 0
16 [FI2011] MHO 2426 B out 18 58 07.0 +01 37 00           ~ 2 0
17 [FI2011] MHO 2423 B out 18 58 07.2 +01 36 52           ~ 2 0
18 MHO 2425 EmO 18 58 07.6 +01 37 30           ~ 2 0
19 [FI2011] MHO 2424 B out 18 58 08.0 +01 36 33           ~ 2 0
20 [AAJ2015] G035.137-00.762 HII 18 58 10 +01 36.9           ~ 2 0
21 AGAL G035.197-00.742 cor 18 58 12.816 +01 40 36.62           ~ 23 0
22 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1

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