2019A&A...622A.135N


Query : 2019A&A...622A.135N

2019A&A...622A.135N - Astronomy and Astrophysics, volume 622A135-135 (2019/2-1)

ATLASGAL-selected massive clumps in the inner Galaxy. VII. Characterisation of mid-J CO emission.

NAVARETE F., LEURINI S., GIANNETTI A., WYROWSKI F., URQUHART J.S., KONIG C., CSENGERI T., GUSTEN R., DAMINELI A. and MENTEN K.M.

Abstract (from CDS):


Context. High-mass stars are formed within massive molecular clumps, where a large number of stars form close together. The evolution of the clumps with different masses and luminosities is mainly regulated by their high-mass stellar content and the formation of such objects is still not well understood.
Aims. In this work, we characterise the mid-J CO emission in a statistical sample of 99 clumps (TOP100) selected from the ATLASGAL survey that are representative of the Galactic proto-cluster population.
Methods. High-spatial resolution APEX-CHAMP+ maps of the CO (6-5) and CO (7-6) transitions were obtained and combined with additional single-pointing APEX-FLASH+ spectra of the CO (4-3) line. The data were convolved to a common angular resolution of 13.4". We analysed the line profiles by fitting the spectra with up to three Gaussian components, classified as narrow or broad, and computed CO line luminosities for each transition. Additionally, we defined a distance-limited sample of 72 sources within 5kpc to check the robustness of our analysis against beam dilution effects. We have studied the correlations of the line luminosities and profiles for the three CO transitions with the clump properties and investigate if and how they change as a function of the evolution.
Results. All sources were detected above 3-σ in all three CO transitions and most of the sources exhibit broad CO emission likely associated with molecular outflows. We find that the extension of the mid-J CO emission is correlated with the size of the dust emission traced by the Herschel-PACS 70 µm maps. The CO line luminosity (LCO) is correlated with the luminosity and mass of the clumps. However, it does not correlate with the luminosity-to-mass ratio.
Conclusions. The dependency of the CO luminosity with the properties of the clumps is steeper for higher-J transitions. Our data seem to exclude that this trend is biased by self-absorption features in the CO emission, but rather suggest that different J transitions arise from different regions of the inner envelope. Moreover, high-mass clumps show similar trends in CO luminosity as lower mass clumps, but are systematically offset towards larger values, suggesting that higher column density and (or) temperature (of unresolved) CO emitters are found inside high-mass clumps.

Abstract Copyright: © ESO 2019

Journal keyword(s): astrochemistry - stars: formation - stars: protostars - ISM: molecules - ISM: kinematics and dynamics - line: profiles

VizieR on-line data: <Available at CDS (J/A+A/622/A135): tablea1.dat-tablea7.dat>

Simbad objects: 105

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Number of rows : 105
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 OH 301.14-00.23 Mas 12 35 35.14 -63 02 32.6           ~ 22 0
2 [HBM2005] G305.192-0.006 cor 13 11 13.6 -62 47 29           ~ 21 0
3 [HBM2005] G305.21+0.21 cor 13 11 14 -62 34.7           ~ 26 0
4 MMB G305.563+00.013 cor 13 14 26.90 -62 44 29.4           ~ 23 0
5 AGAL G305.794-00.096 Y*O 13 16 33.814 -62 49 41.20           ~ 20 0
6 OH 309.39-00.13 Mas 13 47 23.98 -62 18 12.0           ~ 16 0
7 AGAL G310.014+00.387 cor 13 51 40 -61 39.4           ~ 25 0
8 AGAL G313.576+00.324 cor 14 20 08 -60 42.1           ~ 21 0
9 OH 316.64-00.09 Mas 14 44 18.45 -59 55 11.5           ~ 34 0
10 AGAL G317.867-00.151 Y*O 14 53 16.699 -59 26 30.07           ~ 28 0
11 AGAL G318.779-00.137 Y*O 14 59 32.902 -59 00 30.90           ~ 23 0
12 AGAL G320.881-00.397 Y*O 15 14 32.7 -58 11 28           ~ 20 0
13 MMB G326.662+00.520 cor 15 45 02.95 -54 09 03.1           ~ 19 0
14 IRAS 15437-5343 Y*O 15 47 32.73 -53 52 38.4           ~ 68 0
15 MMB G326.986-00.031 Y*O 15 49 07.67 -54 23 04.5           ~ 19 0
16 AGAL G327.393+00.199 cor 15 50 19 -53 57.1           ~ 20 0
17 RCW 97 HII 15 53 05.0 -54 35 24           ~ 171 0
18 AGAL G329.029-00.206 cor 16 00 32 -53 12.9           ~ 18 0
19 AGAL G329.066-00.307 HII 16 01 09.8 -53 16 01           ~ 41 0
20 OH 329.07-00.31 Y*O 16 01 09.999 -53 16 02.94           ~ 38 0
21 MMB G330.953-00.182 cor 16 09 52.37 -51 54 57.6           ~ 40 0
22 AGAL G331.709+00.582 Y*O 16 10 06.61 -50 50 29.0           ~ 27 0
23 OH 330.9-00.3 Mas 16 10 19.80 -52 06 07.9           ~ 18 0
24 IRAS 16124-5110 Y*O 16 16 16.46832 -51 18 25.1964           ~ 47 1
25 IRAS 16157-4957 Y*O 16 19 29.003 -50 04 40.94           ~ 46 0
26 OH 332.826-00.549 Mas 16 20 10.85 -50 53 14.2           ~ 16 0
27 OH 333.14-00.43 Mas 16 21 02.82 -50 35 12.0           ~ 19 0
28 AGAL G333.656+00.059 Y*O 16 21 12.065 -49 52 17.54           ~ 22 0
29 [LCU2014] G333.286-00.387 cor 16 21 30.3 -50 26 48           ~ 29 0
30 AGAL G333.604-00.212 cor 16 22 09.45024 -50 05 58.0920           ~ 49 0
31 OH 335.79+00.17 Mas 16 29 47.309 -48 15 51.77           ~ 42 0
32 MMB G336.957-00.225 cor 16 36 16.9508136648 -47 40 48.064000872           ~ 28 0
33 MMB G337.176-00.032 cor 16 36 18.82 -47 23 19.9           ~ 27 0
34 AGAL G337.286+00.007 cor 16 36 34.207 -47 16 46.03           ~ 22 0
35 OH 337.258-00.101 Mas 16 36 56.32 -47 22 26.4           ~ 12 0
36 AGAL G337.704-00.054 cor 16 38 29.650 -47 00 35.67           ~ 30 0
37 OH 337.40-00.41 Mas 16 38 50.52 -47 28 00.2           ~ 40 0
38 AGAL G338.066+00.044 Y*O 16 39 28.5 -46 40 30           ~ 18 0
39 AGAL G338.786+00.476 Y*O 16 40 21.840 -45 51 06.96           ~ 23 0
40 AGAL G338.926+00.554 cor 16 40 34 -45 41.7           ~ 37 0
41 AGAL G337.916-00.477 cor 16 41 10.6 -47 08 03           ~ 44 0
42 OH 339.6-00.1 Y*O 16 46 05.99 -45 36 43.3           ~ 86 0
43 AGAL G340.374-00.391 Y*O 16 50 01.466 -45 12 36.91           ~ 21 0
44 OH 340.78-00.10 Mas 16 50 14.84 -44 42 26.3           ~ 50 0
45 OH 341.22-00.21 Y*O 16 52 17.92032 -44 26 52.4076           ~ 59 0
46 AGAL G340.746-01.001 cor 16 54 03.66 -45 18 45.1           ~ 18 0
47 MMB G342.484+00.183 cor 16 55 02.30 -43 12 59.8           ~ 29 0
48 [PLW2012] G343.124-00.064-030.4 cor 16 58 17 -42 52.3           ~ 31 0
49 OH 343.756-00.163 Mas 17 00 49.89 -42 26 08.2           ~ 7 0
50 AGAL G345.718+00.817 cor 17 03.1 -40 17           ~ 24 0
51 OH 344.22-00.57 Mas 17 04 07.78 -42 18 39.5           ~ 27 0
52 OH 345.50+00.35 Mas 17 04 22.91 -40 44 21.7           ~ 50 0
53 OH 345.487+00.314 Mas 17 04 28.24 -40 46 28.7           ~ 12 0
54 IRAS 17016-4124 SFR 17 05 11.160 -41 29 06.00           ~ 75 0
55 AGAL G351.131+00.771 Y*O 17 19 34.615 -35 56 48.96           ~ 20 0
56 OH 351.16+00.70 Mas 17 19 57.50 -35 57 52.8           ~ 27 0
57 AGAL G351.244+00.669 cor 17 20 17.84 -35 54 46.0           ~ 35 0
58 AGAL G351.571+00.762 Y*O 17 20 51.168 -35 35 25.70           ~ 31 0
59 AGAL G351.416+00.646 cor 17 20 53 -35 47.0           ~ 29 0
60 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 373 0
61 AGAL G351.444+00.659 cor 17 20 54.60 -35 45 12.8           ~ 35 0
62 MMB G351.581-00.353 cor 17 25 25.220 -36 12 45.34           ~ 44 0
63 AGAL G353.066+00.452 Y*O 17 26 13.330 -34 31 53.52           ~ 26 0
64 OH 351.75-00.53 Mas 17 26 42.57 -36 09 17.6           ~ 74 1
65 AGAL G353.417-00.079 Y*O 17 29 18.94 -34 32 05.9           ~ 22 0
66 AGAL G354.944-00.537 cor 17 35 12.7753 -33 30 22.961           ~ 31 0
67 NAME Sgr B2 (North) Rad 17 47 20.2 -28 22 21           ~ 742 1
68 OH 008.68-00.37 Mas 18 06 23.49 -21 37 10.2           ~ 31 0
69 AGAL G008.706-00.414 Y*O 18 06 37 -21 37.4           ~ 43 0
70 MMB G010.472+00.027 cor 18 08 38.2290 -19 51 50.262           ~ 83 1
71 GAL 010.47+00.03 HII 18 08 38.4 -19 51 52           ~ 159 0
72 OH 010.44-00.02 Mas 18 08 44.88 -19 54 38.2           ~ 18 0
73 MMB G010.627-00.384 cor 18 10 29.22 -19 55 41.1           ~ 65 1
74 MMB G013.179+00.061 cor 18 14 00.96 -17 28 32.5           ~ 33 0
75 AGAL G012.804-00.199 cor 18 14 13.34 -17 55 45.3           ~ 49 0
76 AGAL G014.194-00.194 Y*O 18 16 59 -16 42.2           ~ 40 0
77 AGAL G014.492-00.139 MoC 18 17 22 -16 25.0           ~ 54 0
78 MMB G013.657-00.599 cor 18 17 24.26 -17 22 12.5           ~ 30 0
79 AGAL G014.114-00.574 Y*O 18 18 13 -16 57.4           ~ 35 0
80 MMB G014.631-00.577 cor 18 19 15.21 -16 30 04.5           ~ 27 0
81 AGAL G015.030-00.669 cor 18 20 23 -16 11.4           ~ 28 0
82 NAME IRDC 18223-3 Y*O 18 25 08 -12 45.5           ~ 80 0
83 [CUS2014] G018.7344-0.2261 cor 18 25 56 -12 42.8           ~ 34 0
84 MMB G018.888-00.475 cor 18 27 07.85 -12 41 35.9           ~ 25 0
85 MMB G019.884-00.534 cor 18 29 14.37 -11 50 23.0           ~ 119 1
86 AGAL G022.376+00.447 Y*O 18 30 24 -09 10.6           ~ 47 0
87 AGAL G023.206-00.377 cor 18 34 55 -08 49.3           ~ 36 0
88 AGAL G024.629+00.172 Y*O 18 35 35.6 -07 18 12           ~ 40 0
89 AGAL G028.861+00.066 cor 18 43 46 -03 35.5           ~ 31 0
90 AGAL G028.564-00.236 cor 18 44 17.69 -03 59 26.5           ~ 53 0
91 AGAL G030.893+00.139 cor 18 47 14 -01 45.1           ~ 31 0
92 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 430 1
93 AGAL G030.818-00.056 cor 18 47 47.0 -01 54 28           ~ 186 0
94 AGAL G030.848-00.081 Y*O 18 47 56 -01 53.5           ~ 36 0
95 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 108 0
96 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 537 0
97 AGAL G034.401+00.226 cor 18 53 18.6 +01 24 40           ~ 74 1
98 [CUS2014] G034.2572+0.1535 cor 18 53 18.6449 +01 15 01.574           ~ 43 0
99 RAFGL 5542 Y*O 18 53 37.88832 +01 50 30.5844           ~ 78 0
100 AGAL G035.197-00.742 cor 18 58 12.816 +01 40 36.62           ~ 23 0
101 IRAS 18566+0408 Y*O 18 59 09.95520 +04 12 15.6240           ~ 143 0
102 BGPS G043.169+00.009 cor 19 10 14.2145 +09 06 17.697           ~ 31 0
103 AGAL G049.489-00.389 cor 19 23 44.15 +14 30 29.5           ~ 23 0
104 AGAL G053.141+00.069 cor 19 29 17.50 +17 56 24.0           ~ 33 1
105 MSX6C G059.7831+00.0648 Y*O 19 43 11.2464 +23 44 03.270           ~ 159 0

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