2013A&A...554A..48R


Query : 2013A&A...554A..48R

2013A&A...554A..48R - Astronomy and Astrophysics, volume 554A48-48 (2013/6-1)

The role of low-mass star clusters in massive star formation. The Orion case.

RIVILLA V.M., MARTIN-PINTADO J., JIMENEZ-SERRA I. and RODRIGUEZ-FRANCO A.

Abstract (from CDS):

Different theories have been proposed to explain the formation of massive stars: two are based on accretion processes (monolithic core accretion and competitive accretion), and another on coalescence of low- and intermediate-mass stars. To distinguish between these theories, it is crucial to establish the distribution, the extinction, and the density of young low-mass stars in massive star-forming regions. X-ray observations can penetrate the very obscured cradles of massive stars, directly sampling the distribution of the population of pre-main sequence (PMS) low-mass stars in these regions. Our aim is to analyze deep X-ray observations of the Orion massive star-forming region using the Chandra Orion Ultradeep Project (COUP) catalog, to reveal the distribution of the population and clustering of PMS low-mass stars, and to study their possible role in massive star formation. We studied the distribution of PMS low-mass stars with X-ray emission in Orion as a function of extinction with two different methods: a spatial gridding and a close-neigbors method with cells of ∼0.03x0.03pc2, the typical size of protostellar cores. We derived density maps of the stellar population and calculated cluster stellar densities. Consistent with previous studies, we found that PMS low-mass stars cluster toward the three massive star-forming regions: the Trapezium cluster (TC), the Orion hot core (OHC), and the OMC1-S region. We derived PMS low-mass stellar densities of 105 stars/pc3 in the TC and OMC1-S, and of 106 stars/pc3 in the OHC. The close association between the low-mass star clusters with massive star cradles supports the role of these clusters in the formation of massive stars. The X-ray observations show for the first time in the TC that low-mass stars with intermediate extinction are clustered toward the position of the most massive star θ1 Ori C, which is surrounded by a ring of non-extincted PMS low-mass stars. This ``envelope-core'' structure is also supported by infrared and optical observations. Our analysis suggests that at least two basic ingredients are needed in massive star formation: the presence of dense gas and a cluster of low-mass stars. The scenario that better explains our findings assumes high fragmentation in the parental core, accretion at subcore scales that forms a low-mass stellar cluster, and subsequent competitive accretion. Finally, although coalescence does not seem a common mechanism for building up massive stars, we show that a single stellar merger may have occurred in the evolution of the OHC cluster, favored by the presence of disks, binaries, and gas accretion.

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Journal keyword(s): stars: formation - stars: low-mass - stars: massive - stars: pre-main sequence - ISM: clouds - X-rays: stars

Simbad objects: 14

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Number of rows : 14
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 V* V2254 Ori Or* 05 35 14.11296 -05 22 22.7316           B 320 2
3 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
4 ALMA J053514.3589-052232.733 Y*O 05 35 14.3580 -05 22 32.726           ~ 111 0
5 COUP 622 Y*? 05 35 14.3700 -05 22 36.100     23.30     ~ 25 0
6 NAME OMC 1S PoC 05 35 14.5 -05 25 49           ~ 78 1
7 NAME Orion Core ? 05 35 14.5 -05 22 30           ~ 212 0
8 * tet01 Ori C SB* 05 35 16.4662967280 -05 23 22.921811880 4.20 5.15 5.13 4.91 4.73 O7Vp 1479 1
9 NAME Ori Trapezium OpC 05 35 16.5 -05 23 14           ~ 1708 1
10 NAME Ori Region reg 05 35 17.30 -05 23 28.0           ~ 623 0
11 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1227 1
12 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 789 2
13 NGC 6357 OpC 17 24 44 -34 12.2           ~ 303 0
14 NAME Cep A HW 2 Y*O 22 56 17.9 +62 01 49           B0.5 243 0

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