2024A&A...691A.359L


Query : 2024A&A...691A.359L

2024A&A...691A.359L - Astronomy and Astrophysics, volume 691A359 (2024/11-1)

Observational studies of S-bearing molecules in massive star-forming regions.

LUO R., WANG J.Z., ZHANG X., QUAN D.H., JIANG X.J., LI J., GOU Q., LI Y.Q., XU Y.N., ZHENG S.Q., OU C. and LIU Y.J.

Abstract (from CDS):

Context. S-bearing molecules are powerful tools for determining the physical conditions inside a massive star-forming region. The abundances of S-bearing molecules, including H2S, H2CS, and HCS+, are highly dependent on physical and chemical changes, which means that they are good tracers of the evolutionary stage of massive star formation.
Aims. We present observational results of H2S 110-101, H234S 110-101, H2CS 514-414, HCS+ 4-3, SiO 4-3, HC3N 19-18, and C18O 1-0 toward a sample of 51 late-stage massive star-forming regions, and study the relationships between H2S, H2 CS, HCS+, and SiO in hot cores. We discuss the chemical connections of these S-bearing molecules based on the relations between the relative abundances in our sources.
Methods. H234S 110-101, as the isotopic line of H2S 110-101, was used to correct the optical depths ofH2S 110-101. Beam-averaged column densities of all molecules were calculated, as were the abundances of H2S, H2CS, and HCS+ relative to H2, which were derived from C18 O. Results from a chemical model that included gas, dust grain surface, and icy mantle phases, were compared with the observed abundances of H2S, H2CS, and HCS+ molecules.
Results. H2S 110-101, H234S 110-101, H2CS 514-414, HCS+ 4-3, andHC3N 19-18 were detected in 50 of the 51 sources, SiO 4-3 was detected in 46 sources, and C18O 1-0 was detected in all sources. The Pearson correlation coefficients between H2CS and HCS+ normalized by H2 and H2S are 0.94 and 0.87, respectively, and a tight linear relationship with a slope of 1.00 and 1.09 is found; this relationship is 0.77 and 0.98 between H2S and H2CS and 0.76 and 0.97 between H2S and HCS+. The full widths at half maxima of H234S 110-101, H2CS 514-414, HCS+ 4-3, and HC3N 19-18 in each source are similar to each other, which indicates that they may trace similar regions. By comparing the observed abundance with model results, we see that there is one possible time (2-3 × 105 yr) a which each source in the model matches the measured abundances of H2S, H2CS, and HCS+. The abundances of HCS+, H2CS, and H2S increase with the SiO abundance in these sources, which implies that shock chemistry may be playing a large role.
Conclusions. The close abundance relation of H2S, H2CS, and HCS+ and the similar line widths in observational results indicate that these three molecules could be chemically linked, with HCS+ and H2CS the most correlated. The comparison of the observational results with chemical models shows that the abundances can be reproduced for almost all the sources at a specific time. The observational results, including the abundances in these sources need to be considered in further modeling of H2S, H2CS, and HCS+ in hot cores with shock chemistry.

Abstract Copyright: © The Authors 2024

Journal keyword(s): ISM: abundances - ISM: clouds - ISM: molecules

Simbad objects: 54

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Number of rows : 54
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 LDN 1287 DNe 00 36 47.5 +63 29 02           ~ 103 0
2 [RMB2014] G123.06-06.30a Mas 00 52 24.7008 +56 33 50.527           ~ 5 0
3 NGC 281 HII 00 52 25.1 +56 33 54           ~ 251 1
4 [HMW2016] G133.947+01.064 Mas 02 27 03.8190 +61 52 25.230           ~ 12 0
5 [RMB2014] G168.06+00.82 Mas 05 17 13.7436 +39 22 19.915           ~ 5 0
6 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
7 [RMB2014] G209.00-19.38 Mas 05 35 15.8000 -05 23 14.100           ~ 6 0
8 [RMB2014] G176.51+00.20 Mas 05 37 52.1353 +32 00 03.928           ~ 4 0
9 IRAS 05373+2349 Y*O 05 40 24.2280641304 +23 50 54.705306336           ~ 68 1
10 MMB G188.946+00.886 Mas 06 08 53.3441 +21 38 29.099           ~ 31 0
11 MMB G192.600-00.048 Y*O 06 12 54.0100 +17 59 23.200           ~ 430 0
12 [RMB2014] G211.59+01.05 Mas 06 52 45.3210 +01 40 23.072           ~ 4 0
13 IRAS 07299-1651 Y*O 07 32 09.7800 -16 58 12.800           ~ 85 0
14 OH 328.25-00.53 Mas 15 57 59.75 -53 58 00.4           ~ 69 0
15 NAME Sgr B2N Mas 17 47 20.0000 -28 22 40.000           ~ 49 1
16 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2443 1
17 OH 005.90-00.38 Mas 18 00 30.373 -24 04 00.96           ~ 51 1
18 OH 009.621+00.196 Mas 18 06 14.6600 -20 31 31.700           ~ 56 0
19 MMB G010.472+00.027 cor 18 08 38.2290 -19 51 50.262           ~ 83 1
20 [RMB2014] G010.62-00.38 Mas 18 10 28.5628 -19 55 48.738           ~ 6 0
21 OH 012.889+00.489 Mas 18 11 51.4450 -17 31 29.412           ~ 48 0
22 [HC96] G11.94-0.62 1 Mas 18 13 58.1205 -18 54 20.278           ~ 13 0
23 [RMB2014] G012.81-00.19 Mas 18 14 14.0600 -17 55 11.300           ~ 6 0
24 GAL 012.90-00.24 Mas 18 14 34.4366 -17 51 51.891           ~ 13 0
25 W 33a Y*O 18 14 39.56547 -17 52 02.2260           ~ 746 0
26 IRAS 18134-1942 HII 18 16 22.1327 -19 41 27.219           ~ 72 0
27 [BE83] Maser 014.33-00.64 cor 18 18 54.6744 -16 47 50.264           ~ 24 0
28 OH 015.03-00.68 Mas 18 20 24.8111 -16 11 35.316           ~ 31 1
29 OH 016.59-00.05 Mas 18 21 09.0840 -14 31 48.556           ~ 85 0
30 Caswell CH3OH 023.010-00.411 Mas 18 34 40.2800 -09 00 38.360           ~ 20 0
31 GAL 023.44-00.18 HII 18 34 43.6 -08 32 25           ~ 58 0
32 [HMW2016] G027.365-00.165 Mas 18 41 51.0570 -05 01 43.443           ~ 9 0
33 IRAS 18411-0338 Y*O 18 43 46.2233 -03 35 29.846           ~ 25 0
34 [HMW2016] G029.955-00.016 Mas 18 46 03.7402 -02 39 22.328           ~ 9 0
35 [RMB2014] G031.28+00.06 Mas 18 48 12.3760 -01 26 28.778           ~ 7 0
36 [RMB2014] G031.58+00.07 Mas 18 48 41.6740 -01 09 59.774           ~ 6 0
37 [HMW2016] G032.044+00.059 Mas 18 49 36.5754 -00 45 45.539           ~ 10 0
38 GAL 034.4+00.23 HII 18 53 17.4 +01 24 55           ~ 93 1
39 Caswell OH 035.02+00.35 Mas 18 54 00.6576 +02 01 19.217           ~ 17 0
40 IRAS 18517+0437 SFR 18 54 13.8 +04 41 32           ~ 89 0
41 OH 035.2-00.7 Mas 18 58 13.0517 +01 40 35.674           ~ 49 0
42 OH 035.200-01.736 Mas 19 01 45.5420 +01 13 32.690           ~ 20 0
43 W 49n HII 19 10 13.2 +09 06 12           ~ 497 3
44 OH 043.796-00.127 Mas 19 11 53.9868 +09 35 50.325           ~ 89 0
45 [HMW2016] G049.489-00.369 Mas 19 23 39.8240 +14 31 04.950           ~ 9 0
46 W 51m Rad 19 23.7 +14 30           ~ 72 0
47 MSX6C G059.7831+00.0648 Y*O 19 43 11.2464 +23 44 03.270           ~ 159 0
48 [RMB2014] G069.54-00.97 Mas 20 10 09.0700 +31 31 35.950           ~ 6 0
49 [HMW2016] G078.122+03.632 Mas 20 14 26.0700 +41 13 32.690           ~ 8 0
50 GAL 075.76+00.34 Mas 20 21 41.0860 +37 25 29.280           ~ 30 1
51 [HMW2016] G081.871+00.780 Mas 20 38 36.4260 +42 37 34.800           ~ 10 0
52 MSX6C G081.7522+00.5906 Y*O 20 39 01.9930 +42 24 59.290           ~ 36 0
53 [HLB98] Onsala 150 Mas 21 09 21.7320 +52 22 37.080           ~ 10 0
54 [MBC2000b] J225618.095+620149.45 Mas 22 56 18.0559 +62 01 49.562           ~ 10 0

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