2016A&A...594A.118M


Query : 2016A&A...594A.118M

2016A&A...594A.118M - Astronomy and Astrophysics, volume 594A, 118-118 (2016/10-1)

The structure and early evolution of massive star forming regions. Substructure in the infrared dark cloud SDC13.

McGUIRE C., FULLER G.A., PERETTO N., ZHANG Q., TRAFICANTE A., AVISON A. and JIMENEZ-SERRA I.

Abstract (from CDS):

Context. Investigations into the substructure of massive star forming regions are essential for understanding the observed relationships between core mass distributions and mass distributions in stellar clusters, differentiating between proposed mechanisms of massive star formation.
Aims. We study the substructure in the two largest fragments (i.e. cores) MM1 and MM2, in the infrared dark cloud complex SDC13. As MM1 appears to be in a later stage of evolution than MM2, comparing their substructure provides an insight in to the early evolution of massive clumps.
Methods. We report the results of high resolution SMA dust continuum observations towards MM1 and MM2. Combining these data with Herschel observations, we carry out RADMC-3D radiative transfer modelling to characterise the observed substructure.
Results. SMA continuum data indicates 4 sub-fragments in the SDC13 region. The nature of the second brightest sub-fragment (B) is uncertain as it does not appear as prominent at the lower MAMBO resolution or at radio wavelengths. Statistical analysis indicates that it is unlikely to be a background source, an AGB star, or the free-free emission of a HII region. It is plausible that B is a runaway object ejected from MM1. MM1, which is actively forming stars, consists of two sub-fragments A and C. This is confirmed by 70µm Herschel data. While MM1 and MM2 appear quite similar in previous low resolution observations, at high resolution, the sub-fragment at the centre of MM2 (D) is much fainter than sub-fragment at the centre of MM1 (A). RADMC-3D models of MM1 and MM2 are able to reproduce these results, modelling MM2 with a steeper density profile and higher mass than is required for MM1. The relatively steep density profile of MM2 depends on a significant temperature decrease in its centre, justified by the lack of star formation in MM2. A final stellar population for MM1 was extrapolated, indicating a star formation efficiency typical of regions of core and cluster formation.
Conclusions. The proximity of MM1 and MM2 suggests they were formed at the similar times, however, despite having a larger mass and steeper density profile, the absence of stars in MM2 indicates that it is in an earlier stage of evolution than MM1. This suggests that the density profiles of such cores become shallower as they start to form stars and that evolutionary timescales are not solely dependent on initial mass. Some studies also indicate that the steep density profile of MM2 makes it more likely to form a single massive central object, highlighting the importance of the initial density profile in determining the fragmentation behaviour in massive star forming regions.

Abstract Copyright: © ESO, 2016

Journal keyword(s): stars: formation - ISM: clouds - stars: massive - stars: protostars

Status at CDS : Examining the need for a new acronym.

Simbad objects: 12

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Number of rows : 12
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1311 0
2 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 2981 2
3 SDC G13.158-0.073 DNe 18 14 28.29 -17 33 27.7           ~ 7 0
4 [PFA2014] MM2 mm 18 14 28.53 -17 33 30.9           ~ 4 0
5 [PFA2014] MM18 mm 18 14 29.46 -17 33 13.4           ~ 2 0
6 SDC G13.174-0.070 DNe 18 14 29.55 -17 32 32.1           ~ 6 0
7 [PFA2014] SDC13 DNe 18 14 29.7 -17 32 35           ~ 17 0
8 [PFA2014] MM1 mm 18 14 30.86 -17 33 20.4           ~ 4 0
9 SDC G13.194-0.073 DNe 18 14 32.57 -17 31 33.6           ~ 6 0
10 NAME Dragon Nebula DNe 18 42 50.6 -04 03 30           ~ 150 0
11 NAME Cyg X Cld 20 28 41 +41 10.2           ~ 793 1
12 [MBS2007c] CygX-N40 mm 20 38 59.8 +42 23 43           ~ 6 0

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2023.09.28-16:53:58

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