2009A&A...498..147G


Query : 2009A&A...498..147G

2009A&A...498..147G - Astronomy and Astrophysics, volume 498147-159 (2009/4-4)

Spitzer-IRAC GLIMPSE of high mass protostellar objects. II. SED modelling of a bona fide sample.

GRAVE J.M.C. and KUMAR M.S.N.

Abstract (from CDS):

In a previous work (Paper I, Kumar & Grave, 2007A&A...472..155K) a sample of 380 HMPO targets was studied using the GLIMPSE point source catalog and images. A colour-magnitude analysis of the point sources resulted in the identification of infrared counterparts (IRC) of the (sub)mm cores of HMPO candidates which were considered bona fide targets. We aim to estimate and analyse the physical properties of the infrared counterparts of HMPOs by comparing their spectral energy distributions (SED) with those predicted by radiative transfer accretion models of YSOs. The SED of 68 IRCs are extended beyond the GLIMPSE photometry to the possible limits, from the near-infrared to the millimetre wavelengths, by using the 2MASS, GLIMPSE version 2.0 catalogs, MSX, IRAS and some single dish (and interferometric) (sub)mm data. An online SED fitting tool that uses 2D radiative transfer accretion models of YSOs is employed to fit the observed SED to obtain various physical parameters. The SED of IRCs were fitted by models of massive protostars with a range of masses between 5-42M☉ and ages between 103 and 106-years. The median mass and age are 10M☉ and 104yrs. The observed data favours protostars of low effective temperatures (4000-1000K) with correspondingly large effective photospheres (2-200R☉) for the observed luminosities. The envelopes are large with a mean size of ∼0.2-0.3pc and show a distribution that is very similar to the distribution of the sizes of 8µm nebulae discussed in Paper I. The estimated envelope accretion rates are high with a mean value of 10–3M☉/yr and show a power law dependence on mass with an exponent of 2, suggesting spherical accretion at those scales. Disks are found to exist in most of the sources with a mean mass of 10–1.4±0.7M☉. The observed infrared-millimetre SED of the infrared counterparts of HMPOs are successfully explained with an YSO accretion model. The modelled sources mostly represent proto-B stars although some of them could become O stars in the future. We demonstrate that many of these results may represent a realistic picture of massive star formation, despite some of the discrepant results which may be an effect of the assumptions within the models.

Abstract Copyright: ∼

Journal keyword(s): stars: formation - stars: evolution - ISM: HII regions - infrared: stars

VizieR on-line data: <Available at CDS (J/A+A/498/147): table1.dat>

Nomenclature: Table 1: [GK2009] HHMMm+DDMMmmsN N=68.

Simbad objects: 66

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Number of rows : 66
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 IRAS 13384-6152 IR 13 41 54.3593801472 -62 07 34.384826568           ~ 5 0
2 RAFGL 4176 Y*O 13 43 01.70352 -62 08 51.2304           ~ 163 0
3 [GGB2012] G308.9176+00.1231 HII 13 43 02.1 -62 08 52           ~ 59 0
4 IRAS 13481-6124 Y*O 13 51 37.85568 -61 39 07.5168           ~ 55 0
5 IRAS 13560-6133 IR 13 59 35.3 -61 48 17           ~ 4 0
6 [CH87] 311.489+0.368 HII 14 03 35.9 -61 18 22           ~ 19 0
7 IRAS 14131-6126 IR 14 16 48.5095062552 -61 40 25.762901448           ~ 4 0
8 IRAS 14166-6118 bub 14 20 18.5 -61 31 44           ~ 7 0
9 IRAS 14425-6023 cor 14 46 23.22161 -60 35 46.8822           ~ 25 0
10 IRAS 15246-5612 IR 15 28 32.7 -56 23 00           ~ 12 0
11 IRAS 15347-5518 IR 15 38 36.0 -55 28 07           ~ 6 0
12 IRAS 15506-5325 IR 15 54 32.2 -53 33 53           ~ 5 0
13 IRAS 15519-5430 IR 15 55 50.4667609152 -54 38 59.656961040           ~ 14 0
14 IRAS 15579-5347 IR 16 01 52.54 -53 56 28.3           ~ 7 0
15 IRAS 16061-5048 Cld 16 09 57.3 -50 56 45           ~ 6 0
16 IRAS 16082-5031 IR 16 12 03.2 -50 39 16           ~ 7 0
17 IRAS 16093-5015 IR 16 13 05.2 -50 23 05           ~ 7 0
18 IRAS 16148-5011 SFR 16 18 37.104 -50 18 58.32           ~ 13 0
19 IRAS 16218-4931 IR 16 25 37.9 -49 38 20           ~ 3 0
20 2MASS J16254034-4855155 Y*? 16 25 40.35 -48 55 15.6           ~ 7 0
21 LEDA 101328 G 16 27 03.3 -49 23 59   18.0       ~ 13 0
22 IRAS 16344-4605 mul 16 38 08.6 -46 11 10           ~ 4 0
23 IRAS 16363-4645 mul 16 40 00.5 -46 51 32           ~ 10 0
24 IRAS 16464-4359 HII 16 50 01.0 -44 05 03           ~ 6 0
25 IRAS 16501-4314 mul 16 53 41.0 -43 19 22           ~ 8 0
26 IRAS 16573-4214 bub 17 00 55.4 -42 19 35           ~ 12 0
27 GAL 012.89+00.49 HII 18 11 51.3 -17 31 29           ~ 217 0
28 OH 012.03-00.04 Y*O 18 12 01.8400 -18 31 55.800           ~ 91 0
29 IRAS 18144-1723 IR 18 17 24.4 -17 22 13           ~ 35 0
30 IRAS 18151-1208 Y*O 18 17 58.1254 -12 07 24.893           ~ 114 0
31 IRAS 18159-1550 HII 18 18 47.30 -15 48 57.9           ~ 27 0
32 MMB G019.755-00.128 Y*O 18 27 31.602 -11 45 55.17           ~ 54 0
33 MMB G019.884-00.534 cor 18 29 14.37 -11 50 23.0           ~ 119 1
34 GAL 022.357+00.066 HII 18 31 44.9 -09 22 09           ~ 55 0
35 AGAL G023.264+00.077 cor 18 33 24.00 -08 33 31.0           ~ 43 0
36 IRAS 18308-0841 HII 18 33 32.89 -08 39 18.5           ~ 38 0
37 IRAS 18310-0825 HII 18 33 47.9 -08 23 52           ~ 33 0
38 RAFGL 5515 HII 18 36 29.0 -07 40 33           ~ 35 0
39 AGAL G025.409+00.106 cor 18 37 16 -06 38.6           ~ 57 0
40 GAL 026.60-00.02 HII 18 39 55.9 -05 38 45           ~ 34 1
41 IRAS 18431-0312 HII 18 45 45.5 -03 09 21           ~ 21 0
42 IRAS 18440-0148 cor 18 46 36.56 -01 45 21.2           ~ 65 0
43 IRAS 18445-0222 HII 18 47 10.6 -02 19 08           ~ 31 0
44 IRAS 18447-0229 HII 18 47 23.7 -02 25 55           ~ 23 0
45 AGAL G031.158+00.047 cor 18 48 02.46 -01 33 26.5           ~ 45 0
46 AGAL G029.886-00.781 Y*O 18 48 40 -03 03.9           ~ 33 0
47 IRAS 18472-0022 HII 18 49 50.7 -00 19 09           ~ 18 0
48 IRAS 18488+0000 IR 18 51 24.8 +00 04 19           ~ 32 0
49 RAFGL 5542 Y*O 18 53 37.88832 +01 50 30.5844           ~ 78 0
50 AGAL G034.757+00.024 cor 18 54 40.76 +01 38 05.0           ~ 41 0
51 IRAS 18530+0215 cor 18 55 33.7 +02 19 09           ~ 43 0
52 IRAS 18553+0414 cor 18 57 53.37 +04 18 15.7           ~ 36 0
53 IRAS 18566+0408 Y*O 18 59 09.95520 +04 12 15.6240           ~ 143 0
54 AGAL G039.388-00.141 cor 19 03 45 +05 40.7           ~ 58 1
55 IRAS 19035+0641 Y*O 19 06 01.6288 +06 46 36.140           ~ 84 0
56 [BNM96] 042.096+0.354 Y*O 19 07 00.527 +08 18 44.48           ~ 17 0
57 IRAS 19074+0752 cor 19 09 53.55 +07 57 14.8           ~ 46 0
58 IRAS 19092+0841 Rad 19 11 37.4 +08 46 30           ~ 30 0
59 IRAS 19175+1357 cor 19 19 49.22 +14 02 46.8           ~ 30 0
60 AGAL G051.678+00.719 cor 19 23 59 +16 57.7           ~ 48 0
61 AGAL G053.037+00.112 cor 19 28 55.5 +17 52 00           ~ 50 0
62 IRAS 19282+1814 HII 19 30 28.1 +18 20 53           ~ 38 0
63 MSX6C G059.7831+00.0648 Y*O 19 43 11.2464 +23 44 03.270           ~ 159 0
64 IRAS 19410+2336 SFR 19 43 11.5 +23 44 06           ~ 160 0
65 IRAS 19411+2306 cor 19 43 17.9613824400 +23 14 01.619818008           ~ 49 0
66 MSX6C G059.7654-00.0269 HII 19 43 29.8 +23 40 25           ~ 27 0

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