2024A&A...686A.252B


Query : 2024A&A...686A.252B

2024A&A...686A.252B - Astronomy and Astrophysics, volume 686A252 (2024/6-1)

Complex organic molecules uncover deeply embedded precursors of hot cores An APEX unbiased spectral survey of infrared quiet massive clumps.

BOUSCASSE L., CSENGERI T., WYROWSKI F., MENTEN K.M. and BONTEMPS S.

Abstract (from CDS):

Context. During the process of star formation, the dense gas undergoes significant chemical evolution leading to the emergence of a rich variety of molecules associated with hot cores and hot corinos. However, the physical conditions and the chemical processes involved in this evolution are poorly constrained. In particular, the early phases, corresponding to a stage prior to the emergence of any strong ionising emission from the protostar, are still poorly studied.
Aims. In this work, we provide a full inventory of the emission from complex organic molecules (COMs) to investigate the physical structure and chemical composition of six high-mass protostellar envelopes. We aim to investigate the conditions for the emergence of COMs in hot cores.
Methods. We performed an unbiased spectral survey towards six infrared-quiet massive clumps between 159 GHz and 374 GHz with the APEX 12 m telescope, covering the entire atmospheric windows at 2 mm, 1.2 mm, and 0.8 mm. To identify the spectral lines, we used rotational diagrams and radiative transfer modelling assuming local thermodynamic equilibrium.
Results. We detect up to 11 COMs plus three isotopologues, of which at least five COMs (CH3OH, CH3CN, CH3OCHO, CH3OCH3, and CH3CHO) are detected towards all sources. Towards all the objects, most of the COM emission is found to be cold, with respect to the typical temperatures at which COMs are found, with a temperature of 30 K and extended with a size of ∼0.3 pc. Although the bulk of the gas for our sample of young massive clumps has a cold temperature, we also detect emission from COMs originating from the immediate vicinity of the protostar. This warm component of the envelope is best traced by methanol and methyl cyanide, in particular methyl cyanide traces a compact (∼1″) and the hottest (T ∼200 K) component of the envelope. Only three out of the six sources exhibit a robustly detected hot gas component (T > 100 K) traced by several COMs. We find a gradual emergence of the warm component in terms of size and temperature, together with an increasing molecular complexity, allowing us to establish an evolutionary sequence for our sample based on COMs. While they can already be well characterised by an emerging molecular richness, gas temperatures of COMs in the hot gas and molecular abundances suggest that COMs may become abundant in the gas phase at temperatures below the thermal desorption temperature.
Conclusions. Our findings confirm that the sources of our sample of infrared-quiet massive clumps are in an early evolutionary stage during which the bulk of the gas is cold. The presence of COMs is found to be characteristic of these early evolutionary stages accompanying high-mass star and cluster formation. While the extent of the compact heated regions resembles that of hot cores, the molecular abundances, except for complex cyanides, resemble those of hot corinos and are lower than the peak COM abundances of hot cores. We suggest that the emergence of hot cores is preceded by a phase in which mostly O-bearing COMs appear first with similar abundances to hot corinos albeit with larger source sizes.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: formation - stars: massive - stars: protostars - ISM: abundances - ISM: lines and bands - ISM: molecules

VizieR on-line data: <Available at CDS (J/A+A/686/A252): list.dat fits/*>

Simbad objects: 33

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Number of rows : 33
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 W 3 OH HII 02 27 04.1 +61 52 22           ~ 1064 2
2 IRAS F03226+3033 Y*O 03 25 38.83 +30 44 06.2           ~ 371 0
3 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 513 3
4 [HSW2018] NGC 1333-17 smm 03 29 03.73 +31 16 03.8           ~ 131 0
5 V* V512 Per Or* 03 29 03.7578170808 +31 16 03.947525688           M3.5 419 0
6 [TLL2016] Per-emb-12-B Rad 03 29 10.4270 +31 13 32.099           ~ 9 0
7 [JCC87] IRAS 4A2 Y*O 03 29 10.430 +31 13 32.08           ~ 141 1
8 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
9 NAME IRAS 4B1 South Y*O 03 29 12.06 +31 13 01.7           ~ 47 1
10 JCMTSE J033317.8+310932 cor 03 33 17.85 +31 09 31.9           ~ 140 0
11 [TLL2016] Per-emb-11-A Rad 03 43 57.0650 +32 03 04.788           ~ 12 0
12 [PFG2013] A5142-MM1 mm 05 30 48.031 +33 47 54.64           ~ 19 0
13 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
14 OHIO N 001 Rad 12 03 08.09 +07 15 30.1           ~ 23 1
15 RAFGL 4176 Y*O 13 43 01.70352 -62 08 51.2304           ~ 163 0
16 [BMG2016] Sgr B2(N3) cor 14 47 19.248 -28 22 14.91           ~ 28 0
17 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
18 NAME IRAS 16293-2422B Y*O 16 32 22.63 -24 28 31.8           ~ 352 0
19 [BMG2016] Sgr B2(N4) cor 17 47 19.528 -28 22 32.41           ~ 22 0
20 [QSR2011] Sgr B2(N)-SMA2 cor 17 47 19.885 -28 22 13.29           ~ 114 0
21 [BMG2016] Sgr B2(N1) cor 17 47 19.889 -28 22 18.22           ~ 70 0
22 [BMG2016] Sgr B2(N5) cor 17 47 20.047 -28 22 41.34           ~ 25 0
23 GAL 010.47+00.03 HII 18 08 38.4 -19 51 52           ~ 159 0
24 GAL 012.89+00.49 HII 18 11 51.3 -17 31 29           ~ 217 0
25 LDN 483 DNe 18 17 35 -04 39.8           ~ 359 0
26 [BE83] Maser 014.33-00.64 cor 18 18 54.6744 -16 47 50.264           ~ 24 0
27 GAL 019.61-00.23 HII 18 27 38.0 -11 56 42           ~ 162 0
28 [KKT2016] VLA 12 Y*? 18 30 04.10 -02 03 02.5           ~ 30 0
29 GAL 024.78+00.08 HII 18 36.2 -07 13           ~ 89 0
30 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 430 1
31 IRAS 18517+0437 SFR 18 54 13.8 +04 41 32           ~ 89 0
32 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1
33 GRS G075.78 +00.34 HII 20 21 43.6 +37 26 36           ~ 19 0

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