2020A&A...644A..82M


Query : 2020A&A...644A..82M

2020A&A...644A..82M - Astronomy and Astrophysics, volume 644A82-82 (2020/12-1)

Dense cores in the Seahorse infrared dark cloud: physical properties from modified blackbody fits to the far-infrared-submillimetre spectral energy distributions.

MIETTINEN O.

Abstract (from CDS):


Context. Infrared dark clouds (IRDCs) can be the birth sites of high-mass stars, and hence determining the physical properties of dense cores in IRDCs is useful to constrain the initial conditions and theoretical models of high-mass star formation.
Aims. We aim to determine the physical properties of dense cores in the filamentary Seahorse IRDC G304.74+01.32.
Methods. We used data from the Wide-field Infrared Survey Explorer (WISE), Infrared Astronomical Satellite (IRAS), and Herschel in conjuction with our previous 350 and 870µm observations with the Submillimetre APEX Bolometer Camera (SABOCA) and Large APEX BOlometer CAmera, and constructed the far-IR to submillimetre spectral energy distributions (SEDs) of the cores. The SEDs were fitted using single or two-temperature modified blackbody emission curves to derive the dust temperatures, masses, and luminosities of the cores.
Results. For the 12 analysed cores, which include two IR dark cores (no WISE counterpart), nine IR bright cores, and one HII region, the mean dust temperature of the cold (warm) component, the mass, luminosity, H2 number density, and surface density were derived to be 13.3±1.4K (47.0±5.0K), 113±29M☉, 192±94L☉, (4.3±1.2)x105cm–3, and 0.77±0.19g/cm3, respectively. The HII region IRAS 13039-6108a was found to be the most luminous source in our sample ((1.1±0.4)x103L☉). All the cores were found to be gravitationally bound (i.e. the virial parameter αvir<2). Two out of the nine analysed IR bright cores (22%) were found to follow an accretion luminosity track under the assumptions that the mass accretion rate is 10–5M☉/yr, the stellar mass is 10% of the parent core mass, and the radius of the central star is 5R☉. Most of the remaing ten cores were found to lie within 1 dex below this accretion luminosity track. Seven out of 12 of the analysed cores (58%) were found to lie above the mass-radius thresholds of high-mass star formation proposed in the literature. The surface densities of Σ>0.4g/cm3 derived for these seven cores also exceed the corresponding threshold for high-mass star formation. Five of the analysed cores (42%) show evidence of fragmentation into two components in the SABOCA 350µm image.
Conclusions. In addition to the HII region source IRAS 13039-6108a, some of the other cores in Seahorse also appear to be capable of giving birth to high-mass stars. The 22µm dark core SMM 9 is likely to be the youngest source in our sample that has the potential to form a high-mass star (96±23M☉ within a radius of ∼0.1pc). The dense core population in the Seahorse IRDC has comparable average properties to the cores in the well-studied Snake IRDC G11.11-0.12 (e.g. Tdust and L agree within a factor of ∼1.8); furthermore, the Seahorse, which lies ∼60pc above the Galactic plane, appears to be a smaller (e.g. three times shorter in projection, ∼100 times less massive) version of the Snake. The Seahorse core fragmentation mechanisms appear to be heterogenous, including cases of both thermal and non-thermal Jeans instability. High-resolution follow-up studies are required to address the fragmented cores' genuine potential of forming high-mass stars.

Abstract Copyright: © ESO 2020

Journal keyword(s): stars: formation - ISM: clouds - ISM: individual objects: G304.74+01.32 - infrared: ISM - submillimeter: ISM

Simbad objects: 29

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Number of rows : 29
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 [M2018] SMM 1a cor 13 06 19.380 -61 30 19.32           ~ 2 0
2 [MH2010] SMM1 MoC 13 06 20.5 -61 30 15           ~ 5 0
3 [M2018] SMM 1b cor 13 06 23.360 -61 30 10.37           ~ 2 0
4 [MH2010] SMM2 MoC 13 06 26.9 -61 29 39           ~ 5 0
5 [BBC2006] IRAS 13039-6108 Clump 1 cor 13 06 35.8 -61 28 53           ~ 5 0
6 MSXDC G304.74+01.32 DNe 13 06.6 -61 30           ~ 10 0
7 [M2018] BLOB 2 cor 13 06 40.440 -61 29 52.84           ~ 3 0
8 [M2018] BLOB 1 cor 13 06 40.460 -61 29 20.84           ~ 3 0
9 [M2018] SMM 4c cor 13 06 42.860 -61 28 33.03           ~ 2 0
10 [BBC2006] IRAS 13039-6108 Clump 3 cor 13 06 44.7 -61 28 35           ~ 5 0
11 [M2018] SMM 4a cor 13 06 46.210 -61 28 48.04           ~ 2 0
12 [M2018] SMM 4b cor 13 06 46.840 -61 28 22.54           ~ 2 0
13 [MH2010] SMM5 MoC 13 06 49.9 -61 26 55           ~ 5 0
14 IRAS 13037-6112 HII 13 06 51.0 -61 28 22           ~ 8 0
15 [BBC2006] IRAS 13039-6108 Clump 4 cor 13 06 51.1 -61 27 49           ~ 5 0
16 [M2018] IRAS 13037-6112b cor 13 06 51.240 -61 27 51.04           ~ 2 0
17 [M2018] IRAS 13037-6112a cor 13 06 51.450 -61 28 24.04           ~ 2 0
18 [M2018] SMM 6b cor 13 06 52.080 -61 27 40.54           ~ 2 0
19 [M2018] SMM 6a cor 13 06 55.420 -61 27 27.03           ~ 2 0
20 [BBC2006] IRAS 13039-6108 Clump 8 cor 13 07 02.6 -61 26 18           ~ 5 0
21 IRAS 13039-6108 MIR 13 07 06.4 -61 24 29           ~ 11 0
22 [M2018] IRAS 13039-6108a cor 13 07 06.490 -61 24 32.98           ~ 2 0
23 [M2018] IRAS 13039-6108b cor 13 07 08.580 -61 23 56.97           ~ 2 0
24 [MH2010] SMM8 MoC 13 07 08.9 -61 22 49           ~ 5 0
25 [BBC2006] IRAS 13039-6108 Clump 6 cor 13 07 12.7 -61 22 49           ~ 7 0
26 IRAS 13042-6105 MIR 13 07 20.3 -61 21 45           ~ 6 0
27 NAME Gal Center Snake Rad 17 44 17.9 -29 46 00           ~ 62 1
28 [CCE98b] 011.11-0.12 Cld 18 10.5 -19 23           ~ 119 2
29 NAME Dragon Nebula DNe 18 42 50.6 -04 03 30           ~ 177 0

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