2021A&A...652A..71S


Query : 2021A&A...652A..71S

2021A&A...652A..71S - Astronomy and Astrophysics, volume 652A71-71 (2021/8-1)

Establishing the evolutionary timescales of the massive star formation process through chemistry.

SABATINI G., BOVINO S., GIANNETTI A., GRASSI T., BRAND J., SCHISANO E., WYROWSKI F., LEURINI S. and MENTEN K.M.

Abstract (from CDS):


Context. Understanding the details of the formation process of massive (i.e. M≥8-10M☉) stars is a long-standing problem in astrophysics. They form and evolve very quickly, and almost their entire formation process takes place deeply embedded in their parental clumps. Together with the fact that these objects are rare and at a relatively large distance, this makes observing them very challenging.
Aims. We present a method for deriving accurate timescales of the evolutionary phases of the high-mass star formation process.
Methods. We modelled a representative number of massive clumps of the ATLASGAL-TOP100 sample that cover all the evolutionary stages. The models describe an isothermal collapse and the subsequent warm-up phase, for which we followed the chemical evolution. The timescale of each phase was derived by comparing the results of the models with the properties of the sources of the ATLASGAL-TOP100 sample, taking into account the mass and luminosity of the clumps, and the column densities of methyl acetylene (CH3CCH), acetonitrile (CH3CN), formaldehyde (H2CO), and methanol (CH3OH).
Results. We find that the molecular tracers we chose are affected by the thermal evolution of the clumps, showing steep ice evaporation gradients from 103 to 105AU during the warm-up phase. We succeed in reproducing the observed column densities of CH3CCH and CH3CN, but H2CO and CH3OH agree less with the observed values. The total (massive) star formation time is found to be ∼5.2x105yr, which is defined by the timescales of the individual evolutionary phases of the ATLASGAL-TOP100 sample: ∼5x104yr for 70-µm weak, ∼1.2x105yr for mid-IR weak, ∼2.4x105yr for mid-IR bright, and ∼1.1x105yr for HII-region phases.
Conclusions. With an appropriate selection of molecular tracers that can act as chemical clocks, our model allows obtaining robust estimates of the duration of the individual phases of the high-mass star formation process. It also has the advantage of being capable of including additional tracers aimed at increasing the accuracy of the estimated timescales.

Abstract Copyright: © ESO 2021

Journal keyword(s): stars: formation - stars: massive - stars: evolution - astrochemistry - ISM: molecules - evolution

Simbad objects: 50

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Number of rows : 50
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 MMB G305.563+00.013 cor 13 14 26.90 -62 44 29.4           ~ 23 0
4 AGAL G310.014+00.387 cor 13 51 40 -61 39.4           ~ 25 0
5 OH 313.577+00.325 Mas 14 20 08.58 -60 42 00.8           ~ 8 0
6 OH 316.64-00.09 Mas 14 44 18.45 -59 55 11.5           ~ 34 0
7 AGAL G317.867-00.151 Y*O 14 53 16.699 -59 26 30.07           ~ 28 0
8 AGAL G318.779-00.137 Y*O 14 59 32.902 -59 00 30.90           ~ 23 0
9 MMB G326.986-00.031 Y*O 15 49 07.67 -54 23 04.5           ~ 19 0
10 MMB G330.953-00.182 cor 16 09 52.37 -51 54 57.6           ~ 40 0
11 AGAL G331.709+00.582 Y*O 16 10 06.61 -50 50 29.0           ~ 27 0
12 OH 330.9-00.3 Mas 16 10 19.80 -52 06 07.9           ~ 18 0
13 IRAS 16157-4957 Y*O 16 19 29.003 -50 04 40.94           ~ 46 0
14 OH 332.826-00.549 Mas 16 20 10.85 -50 53 14.2           ~ 16 0
15 [LCU2014] G333.286-00.387 cor 16 21 30.3 -50 26 48           ~ 29 0
16 AGAL G333.604-00.212 cor 16 22 09.45024 -50 05 58.0920           ~ 49 0
17 MMB G336.957-00.225 cor 16 36 16.9508136648 -47 40 48.064000872           ~ 28 0
18 OH 337.258-00.101 Mas 16 36 56.32 -47 22 26.4           ~ 12 0
19 OH 339.6-00.1 Y*O 16 46 05.99 -45 36 43.3           ~ 86 0
20 OH 341.22-00.21 Y*O 16 52 17.92032 -44 26 52.4076           ~ 59 0
21 AGAL G340.746-01.001 cor 16 54 03.66 -45 18 45.1           ~ 18 0
22 MMB G342.484+00.183 cor 16 55 02.30 -43 12 59.8           ~ 29 0
23 AGAL G345.718+00.817 cor 17 03.1 -40 17           ~ 24 0
24 OH 345.50+00.35 Mas 17 04 22.91 -40 44 21.7           ~ 50 0
25 AGAL G351.571+00.762 Y*O 17 20 51.168 -35 35 25.70           ~ 31 0
26 AGAL G351.416+00.646 cor 17 20 53 -35 47.0           ~ 29 0
27 AGAL G353.066+00.452 Y*O 17 26 13.330 -34 31 53.52           ~ 26 0
28 OH 351.75-00.53 Mas 17 26 42.57 -36 09 17.6           ~ 74 1
29 AGAL G353.417-00.079 Y*O 17 29 18.94 -34 32 05.9           ~ 22 0
30 OH 353.41-00.36 Mas 17 30 26.18 -34 41 45.6           ~ 65 0
31 AGAL G354.944-00.537 cor 17 35 12.7753 -33 30 22.961           ~ 31 0
32 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
33 AGAL G008.684-00.367 cor 18 06 23.460 -21 37 09.79           ~ 23 0
34 AGAL G008.706-00.414 Y*O 18 06 37 -21 37.4           ~ 43 0
35 OH 010.44-00.02 Mas 18 08 44.88 -19 54 38.2           ~ 18 0
36 MMB G010.627-00.384 cor 18 10 29.22 -19 55 41.1           ~ 65 1
37 MMB G013.179+00.061 cor 18 14 00.96 -17 28 32.5           ~ 33 0
38 AGAL G012.804-00.199 cor 18 14 13.34 -17 55 45.3           ~ 49 0
39 AGAL G014.492-00.139 MoC 18 17 22 -16 25.0           ~ 54 0
40 AGAL G014.114-00.574 Y*O 18 18 13 -16 57.4           ~ 35 0
41 MMB G014.631-00.577 cor 18 19 15.21 -16 30 04.5           ~ 27 0
42 AGAL G024.629+00.172 Y*O 18 35 35.6 -07 18 12           ~ 40 0
43 AGAL G028.564-00.236 cor 18 44 17.69 -03 59 26.5           ~ 53 0
44 AGAL G030.893+00.139 cor 18 47 14 -01 45.1           ~ 31 0
45 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 430 1
46 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 108 0
47 AGAL G034.401+00.226 cor 18 53 18.6 +01 24 40           ~ 74 1
48 AGAL G035.197-00.742 cor 18 58 12.816 +01 40 36.62           ~ 23 0
49 MSX6C G059.7831+00.0648 Y*O 19 43 11.2464 +23 44 03.270           ~ 159 0
50 RAFGL 2591 Y*O 20 29 24.8230 +40 11 19.590           ~ 640 0

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