2013A&A...553A.115B


Query : 2013A&A...553A.115B

2013A&A...553A.115B - Astronomy and Astrophysics, volume 553A115-115 (2013/5-1)

Fragmentation and dynamical collapse of the starless high-mass star-forming region IRDC 18310-4.

BEUTHER H., LINZ H., TACKENBERG J., HENNING T., KRAUSE O., RAGAN S., NIELBOCK M., LAUNHARDT R., BIHR S., SCHMIEDEKE A., SMITH R. and SAKAI T.

Abstract (from CDS):

Because of their short evolutionary time-scales, the earliest stages of high-mass star formation prior to the existence of any embedded heating source have barely been characterized until today. We study the fragmentation and dynamical properties of a massive starless gas clump at the onset of high-mass star formation. Based on Herschel continuum data we identify a massive gas clump that remains far-infrared dark up to 100µm wavelengths. The fragmentation and dynamical properties are investigated by means of Plateau de Bure Interferometer and Nobeyama 45m single-dish spectral line and continuum observations. The massive gas reservoir (between ∼800 and ∼1600M☉, depending on the assumed dust properties) fragments at spatial scales of ∼18000AU in four cores. Comparing the spatial extent of this high-mass region with intermediate- to low-mass starless cores from the literature, we find that linear sizes do not vary significantly over the whole mass regime. However, the high-mass regions squeeze much more gas into these similar volumes and hence have orders of magnitude larger densities. The fragmentation properties of the presented low-to high-mass regions are consistent with gravitational instable Jeans fragmentation. Furthermore, we find multiple velocity components associated with the resolved cores. Recent radiative transfer hydrodynamic simulations of the dynamic collapse of massive gas clumps also result in multiple velocity components along the line of sight because of the clumpy structure of the regions. This result is supported by a ratio between viral and total gas mass for the whole region <1. This apparently still starless high-mass gas clump exhibits clear signatures of early fragmentation and dynamic collapse prior to the formation of an embedded heating source. A comparison with regions of lower mass reveals that the linear size of star-forming regions does not necessarily have to vary much for different masses, however, the mass reservoirs and gas densities are orders of magnitude enhanced for high-mass regions compared to their lower-mass siblings.

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Journal keyword(s): stars: early-type - stars: formation - stars: individual: IRDC18310-4 - stars: massive - ISM: kinematics and dynamics - ISM: clouds

VizieR on-line data: <Available at CDS (J/A+A/553/A115): list.dat fits/*>

Nomenclature: NAME IRDC 18310-4. Fig. 2, Table 2: [BLT2013] mmN (Nos mm1-mm4).

CDS comments: Paragraph 4.2 G11.11 is probably GAL 011.11-00.12.

Simbad objects: 17

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Number of rows : 17
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 NAME Orion Nebula Cluster OpC 05 35.0 -05 29           ~ 2514 0
2 NGC 2264 OpC 06 40 53.7 +09 52 32           ~ 1876 0
3 LDN 57 DNe 17 22 38.2 -23 49 34           ~ 336 1
4 NAME the Pipe Nebula DNe 17 30 -25.0           ~ 442 1
5 [CCE98b] 011.11-0.12 Cld 18 10.5 -19 23           ~ 119 2
6 ICRF J183005.9+061915 Bla 18 30 05.93984953 +06 19 15.9522412       19.5   ~ 124 1
7 PMN J1832-1035 rG 18 32 20.83647 -10 35 11.1968           ~ 107 1
8 [BLT2013] mm2 cor 18 33 39.277 -08 21 09.83           ~ 2 0
9 [BLT2013] mm3 cor 18 33 39.334 -08 21 16.71           ~ 2 0
10 NAME IRDC 18310-4 cor 18 33 39.42 -08 21 10.4           ~ 20 0
11 [BLT2013] mm1 cor 18 33 39.472 -08 21 09.96           ~ 2 0
12 [BLT2013] mm4 cor 18 33 40.013 -08 21 04.84           ~ 2 0
13 IRAS 18310-0825 HII 18 33 47.9 -08 23 52           ~ 33 0
14 W 43 SFR 18 47 32 -01 56.5           ~ 604 0
15 SDC G30.854-0.109 cor 18 48 02.17 -01 53 56.5           ~ 11 0
16 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 837 0
17 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2

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