2024A&A...692A.265S


Query : 2024A&A...692A.265S

2024A&A...692A.265S - Astronomy and Astrophysics, volume 692A265 (2024/12-1)

Time evolution of o-H2D+, N2D+, and N2H+ during the high-mass star formation process.

SABATINI G., BOVINO S., REDAELLI E., WYROWSKI F., URQUHART J.S., GIANNETTI A., BRAND J. and MENTEN K.M.

Abstract (from CDS):

Context. Deuterium fractionation is a well-established evolutionary tracer in low-mass star formation, but its applicability to the high-mass regime remains an open question. In this context, the abundances and ratios of different deuterated species have often been proposed as reliable evolutionary indicators for different stages of the high-mass star formation process.
Aims. In this study, we investigate the role of N2H+ and key deuterated molecules (o-H2D+ and N2D+) as tracers of the different stages of the high-mass star formation process. We assess whether their abundance ratios can serve as reliable evolutionary indicators.
Methods. We conducted APEX observations of o-H2D+ (110-111), N2H+ (4-3), and N2D+ (3-2) in a sample of 40 high-mass clumps at different evolutionary stages, selected from the ATLASGAL survey. Molecular column densities and abundances relative to H2, X, were derived through spectral line modelling, both under local thermodynamic equilibrium (LTE) and non-LTE conditions.
Results. The o-H2D+ column densities show the smallest deviation from LTE conditions when derived under non-LTE assumptions. In contrast, N2H+ shows the largest discrepancy between the column densities derived from LTE and non-LTE. In all the cases discussed, we found that X(o-H2D+) decreases more significantly with each respective evolutionary stage than in the case of X(N2D+); whereas X(N2H+) increases slightly. Therefore, the validity of the X(o-H2D+)/X(N2D+) ratio as a reliable evolutionary indicator, recently proposed as a promising tracer of the different evolutionary stages, was not observed for this sample. While the deuteration fraction derived from N2D+ and N2H+ clearly decreases with clump evolution, the interpretation of this trend is complex, given the different distribution of the two tracers.
Conclusions. Our results suggest that a careful consideration of the observational biases and beam-dilution effects are crucial for an accurate interpretation of the evolution of the deuteration process during the high-mass star formation process.

Abstract Copyright: © The Authors 2024

Journal keyword(s): astrochemistry - molecular processes - stars: formation - evolution

Simbad objects: 37

goto Full paper

goto View the references in ADS

Number of rows : 37
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 Ori B9 Cloud Cld 05 42 30.5 -01 20 33           ~ 26 0
2 [HBM2005] G305.192-0.006 cor 13 11 13.6 -62 47 29           ~ 21 0
3 AGAL G310.014+00.387 cor 13 51 40 -61 39.4           ~ 25 0
4 AGAL G317.867-00.151 Y*O 14 53 16.699 -59 26 30.07           ~ 28 0
5 AGAL G318.779-00.137 Y*O 14 59 32.902 -59 00 30.90           ~ 23 0
6 MMB G326.986-00.031 Y*O 15 49 07.67 -54 23 04.5           ~ 19 0
7 IRAS 16157-4957 Y*O 16 19 29.003 -50 04 40.94           ~ 46 0
8 AGAL G335.789+00.174 cor 16 29 47.189 -48 15 50.23           ~ 28 0
9 AGAL G337.916-00.477 cor 16 41 10.6 -47 08 03           ~ 44 0
10 OH 339.6-00.1 Y*O 16 46 05.99 -45 36 43.3           ~ 86 0
11 OH 341.22-00.21 Y*O 16 52 17.92032 -44 26 52.4076           ~ 59 0
12 AGAL G343.756-00.164 cor 17 00 49.836 -42 26 09.39           ~ 24 0
13 AGAL G345.718+00.817 cor 17 03.1 -40 17           ~ 24 0
14 OH 344.22-00.57 Mas 17 04 07.78 -42 18 39.5           ~ 27 0
15 OH 345.50+00.35 Mas 17 04 22.91 -40 44 21.7           ~ 50 0
16 AGAL G351.131+00.771 Y*O 17 19 34.615 -35 56 48.96           ~ 20 0
17 AGAL G351.161+00.697 cor 17 19 57 -35 57.8           ~ 22 0
18 AGAL G351.244+00.669 cor 17 20 17.84 -35 54 46.0           ~ 35 0
19 AGAL G351.571+00.762 Y*O 17 20 51.168 -35 35 25.70           ~ 31 0
20 AGAL G351.444+00.659 cor 17 20 54.60 -35 45 12.8           ~ 35 0
21 AGAL G353.066+00.452 Y*O 17 26 13.330 -34 31 53.52           ~ 26 0
22 AGAL G353.409-00.361 cor 17 30 26.2 -34 41 46           ~ 27 0
23 AGAL G354.944-00.537 cor 17 35 12.7753 -33 30 22.961           ~ 31 0
24 AGAL G012.496-00.222 cor 18 13 42 -18 12.7           ~ 23 0
25 MMB G013.179+00.061 cor 18 14 00.96 -17 28 32.5           ~ 33 0
26 AGAL G014.194-00.194 Y*O 18 16 59 -16 42.2           ~ 40 0
27 AGAL G014.492-00.139 MoC 18 17 22 -16 25.0           ~ 54 0
28 AGAL G014.114-00.574 Y*O 18 18 13 -16 57.4           ~ 35 0
29 MMB G014.631-00.577 cor 18 19 15.21 -16 30 04.5           ~ 27 0
30 AGAL G015.030-00.669 cor 18 20 23 -16 11.4           ~ 28 0
31 AGAL G015.718-00.594 Y*O 18 21 26.818 -15 33 02.89           ~ 14 0
32 MMB G019.884-00.534 cor 18 29 14.37 -11 50 23.0           ~ 119 1
33 AGAL G022.376+00.447 Y*O 18 30 24 -09 10.6           ~ 47 0
34 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 108 0
35 RAFGL 5542 Y*O 18 53 37.88832 +01 50 30.5844           ~ 78 0
36 [DLW84] G35.2N HII 18 58 13.036 +01 40 36.00           ~ 138 0
37 AGAL G053.141+00.069 cor 19 29 17.50 +17 56 24.0           ~ 33 1

To bookmark this query, right click on this link: simbad:objects in 2024A&A...692A.265S and select 'bookmark this link' or equivalent in the popup menu