2021A&A...645A.142A


Query : 2021A&A...645A.142A

2021A&A...645A.142A - Astronomy and Astrophysics, volume 645A, 142-142 (2021/1-1)

Continuity of accretion from clumps to Class 0 high-mass protostars in SDC335.

AVISON A., FULLER G.A., PERETTO N., DUARTE-CABRAL A., ROSEN A.L., TRAFICANTE A., PINEDA J.E., GUSTEN R. and CUNNINGHAM N.

Abstract (from CDS):


Context. The infrared dark cloud (IRDC) SDC335.579-0.292 (hereafter, SDC335) is a massive (∼5000M) star-forming cloud which has been found to be globally collapsing towards one of the most massive star forming cores in the Galaxy, which is located at its centre. SDC335 is known to host three high-mass protostellar objects at early stages of their evolution and archival ALMA Cycle 0 data (at ∼5'' resolution) indicate the presence of at least one molecular outflow in the region detected in HNC. Observations of molecular outflows from massive protostellar objects allow us to estimate the accretion rates of the protostars as well as to assess the disruptive impact that stars have on their natal clouds during their formation.
Aims. The aim of this work is to identify and analyse the properties of the protostellar-driven molecular outflows within SDC335 and use these outflows to help refine the properties of the young massive protostars in this cloud.
Methods. We imaged the molecular outflows in SDC335 using new data from the Australia Telescope Compact Array of SiO and Class I CH3OH maser emission (at a resolution of ∼3'') alongside observations of four CO transitions made with the Atacama Pathfinder EXperiment and archival Atacama Large Millimeter/submillimeter Array (ALMA) CO, 13CO (∼1''), and HNC data. We introduced a generalised argument to constrain outflow inclination angles based on observed outflow properties. We then used the properties of each outflow to infer the accretion rates on the protostellar sources driving them. These accretion properties allowed us to deduce the evolutionary characteristics of the sources. Shock-tracing SiO emission and CH3OH Class I maser emission allowed us to locate regions of interaction between the outflows and material infalling to the central region via the filamentary arms of SDC335.
Results. We identify three molecular outflows in SDC335 - one associated with each of the known compact HII regions in the IRDC. These outflows have velocity ranges of ∼10km/s and temperatures of ∼60K. The two most massive sources (separated by ∼9000 AU) have outflows with axes which are, in projection, perpendicular. A well-collimated jet-like structure with a velocity gradient of ∼155km/s/pc is detected in the lobes of one of the outflows. The outflow properties show that the SDC335 protostars are in the early stages (Class 0) of their evolution, with the potential to form stars in excess of 50M. The measured total accretion rate, inferred from the outflows, onto the protostars is 1.4(±0.1)x10–3M/yr, which is comparable to the total mass infall rate toward the cloud centre on parsec scales of 2.5(±1.0)x10–3M/yr, suggesting a near-continuous flow of material from cloud to core scales. Finally, we identify multiple regions where the outflows interact with the infalling material in the cloud's six filamentary arms, creating shocked regions and pumping Class I methanol maser emission. These regions provide useful case studies for future investigations of the disruptive effect of young massive stars on their natal clouds.

Abstract Copyright: © A. Avison et al. 2021

Journal keyword(s): stars: formation - ISM: jets and outflows - stars: massive - stars: protostars - ISM: clouds - masers

VizieR on-line data: <Available at CDS (J/A+A/645/A142): listsp.dat spectra/* list.dat fits/*>

CDS comments: Calibrators J1427-4026 and 1646-50 not identified.

Simbad objects: 33

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Number of rows : 33
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 LDN 1448 DNe 03 22.5 +30 35           ~ 515 0
2 LDN 1455M DNe 03 27 48 +30 12.1           ~ 5 0
3 IRAS 03282+3035 cor 03 31 20.98 +30 45 30.1           ~ 176 0
4 HH 211 Y*O 03 43 56.52 +32 00 52.8           ~ 368 0
5 HH 243 HH 05 32 27.83 +12 53 14.6   17.0       ~ 117 0
6 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1619 1
7 IRAS 05358+3543 Y*O 05 39 09.92 +35 45 17.2           ~ 163 0
8 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3042 2
9 QSO B1334-127 Bla 13 37 39.78278132 -12 57 24.6933925   18.5 19.00 16.22   ~ 503 1
10 QSO B1424-41 QSO 14 27 56.29756617 -42 06 19.4376238   18.48 17.7 16.30   ~ 495 1
11 QSO B1514-24 BLL 15 17 41.8134049824 -24 22 19.482207024   15.13 14.00 13.95   ~ 769 3
12 PMN J1604-4227 cm 16 04 47.59969 -42 28 09.4607           ~ 10 0
13 ICRF J161717.8-584807 AGN 16 17 17.89125660 -58 48 07.8601409   18.23       ~ 139 1
14 NAME VLA 1623-243 Y*O 16 26 26.42 -24 24 30.0           ~ 404 0
15 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3629 1
16 [PFD2013] F6 ? 16 29 30.0 -48 44 00           ~ 3 0
17 [PFD2013] F5 ? 16 30 30.0 -48 45 00           ~ 3 0
18 [PFD2013] F1 ? 16 30 30.0 -48 41 00           ~ 3 0
19 [PFD2013] MM2 cor 16 30 57.26 -48 43 39.7           ~ 4 0
20 SDC G335.579-0.292 DNe 16 30 58.00 -48 44 16.3           ~ 33 0
21 [PFD2013] MM1b ? 16 30 58.638 -48 43 51.70           ~ 5 0
22 [PFD2013] MM1 cor 16 30 58.76 -48 43 53.4           ~ 9 0
23 [PFD2013] MM1a ? 16 30 58.765 -48 43 54.00           ~ 5 0
24 [PFD2013] F4 ? 16 31 20.0 -48 45 00           ~ 3 0
25 [PFD2013] F3 ? 16 31 30.0 -48 44 20           ~ 3 0
26 [PFD2013] F2 ? 16 31 35.0 -48 43 30           ~ 3 0
27 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1252 1
28 ICRF J165016.6-504448 QSO 16 50 16.62710806 -50 44 48.2106956   20.95       ~ 76 2
29 AGAL G028.344+00.061 cor 18 42 50.45 -04 03 17.7           ~ 86 0
30 [DLW84] G35.2N HII 18 58 13.036 +01 40 36.00           ~ 116 0
31 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 868 0
32 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1225 1
33 NAME K 3-50A HII 20 01 45.6 +33 32 42           ~ 80 0

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