2014A&A...562A...3M


Query : 2014A&A...562A...3M

2014A&A...562A...3M - Astronomy and Astrophysics, volume 562A, 3-3 (2014/2-1)

A MALT90 study of the chemical properties of massive clumps and filaments of infrared dark clouds.

MIETTINEN O.

Abstract (from CDS):

Infrared dark clouds (IRDCs) provide a useful testbed in which to investigate the genuine initial conditions and early stages of massive-star formation. We attempt to characterise the chemical properties of a sample of 35 massive clumps of IRDCs through multi-molecular line observations. We also search for possible evolutionary trends among the derived chemical parameters. The clumps are studied using the MALT90 (Millimetre Astronomy Legacy Team 90GHz) line survey data obtained with the Mopra 22m telescope. The survey covers 16 different transitions near 90GHz. The spectral-line data are used in concert with our previous LABOCA (Large APEX BOlometer CAmera) 870µm dust emission data. Eleven MALT90 transitions are detected towards the clumps at least at the 3σ level. Most of the detected species (SiO, C2H, HNCO, HCN, HCO+, HNC, HC3N, and N2H+) show spatially extended emission towards many of the sources. Most of the fractional abundances of the molecules with respect to H2 are found to be comparable to those determined in other recent similar studies of IRDC clumps. We found that the abundances of SiO, HNCO, and HCO+ are higher in IR-bright clumps than in IR-dark sources, reflecting a possible evolutionary trend. A hint of this trend is also seen for HNC and HC3N. An opposite trend is seen for the C2H and N2H+ abundances. Moreover, a positive correlation is found between the abundances of HCO+ and HNC, and between those of HNC and HCN. The HCN and HNC abundances also appear to increase as a function of the N2H+ abundance. The HNC/HCN and N2H+/HNC abundance ratios are derived to be near unity on average, while that of HC3N/HCN is ∼10%. The N2H+/HNC ratio appears to increase as the clump evolves, while the HNC/HCO+ ratio shows the opposite behaviour. The detected SiO emission is probably caused by shocks driven by outflows in most cases, although shocks resulting from the cloud formation process could also play a role. Shock-origin for the HNCO, HC3N, and CH3CN emission is also plausible. The average HNC/HCN ratio is in good agreement with those seen in other IRDCs, but gas temperature measurements would be neeeded to study its temperature dependence. Our results support the finding that C2H can trace the cold gas, and not just the photodissociation regions. The HC3N/HCN ratio appears to be comparable to the values seen in other types of objects, such as T Tauri disks and comets.

Abstract Copyright:

Journal keyword(s): astrochemistry - stars: formation - ISM: abundances - ISM: clouds - ISM: molecules - radio lines: ISM

CDS comments: Paragraph 4.8 G034.43 MM1 is [RJS2006] MSXDC G034.43+00.24 MM1 in SIMBAD.

Simbad objects: 57

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Number of rows : 57
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* DM Tau Or* 04 33 48.7336763736 +18 10 09.973460280 14.30 14.82 14.00     M2Ve 633 0
2 EM* LkCa 15 Or* 04 39 17.7911622816 +22 21 03.390090984   13.01 12.03 11.61   K5:Ve 690 1
3 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1676 0
4 HD 31648 Ae* 04 58 46.2655706952 +29 50 36.987625680 7.84 7.78 7.62 7.76 7.43 A5Vep 518 0
5 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1098 1
6 RCW 97 HII 15 53 05.0 -54 35 24           ~ 157 0
7 LDN 183 MoC 15 54 12.2 -02 49 42           ~ 759 1
8 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1252 1
9 NAME Nessie Nebula DNe 16 43 -46.7           ~ 27 0
10 NGC 6334E HII 17 20 50.9 -35 46 06           ~ 52 0
11 NGC 6334 HII 17 20 53 -36 07.9           ~ 682 0
12 IRAS 17233-3606 HII 17 26 42.8 -36 09 17           ~ 84 0
13 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2266 1
14 AGAL G001.647-00.062 DNe 17 49 44 -27 33.5           ~ 11 0
15 MMB G001.719-00.088 Mas 17 49 59.84 -27 30 36.9           ~ 12 0
16 [M2012] G001.87-00.14 SMM 8 DNe 17 50 00.6665 -27 29 23.966           ~ 6 0
17 [M2012] G001.87-00.14 SMM 11 smm 17 50 02.1 -27 34 28           ~ 2 0
18 AGAL G001.674-00.127 smm 17 50 03 -27 33.7           ~ 8 0
19 [M2012] G001.87-00.14 SMM 14 DNe 17 50 04.2 -27 34 57           ~ 2 0
20 [M2012] G001.87-00.14 SMM 15 smm 17 50 05.234 -27 28 22.40           ~ 6 0
21 AGAL G001.696-00.142 DNe 17 50 09 -27 33.4           ~ 8 0
22 [M2012] G001.87-00.14 SMM 17 DNe 17 50 12.3 -27 36 48           ~ 2 0
23 [M2012] G001.87-00.14 SMM 20 smm 17 50 13.5 -27 20 40           ~ 2 0
24 [M2012] G001.87-00.14 SMM 21 smm 17 50 13.8 -27 35 24           ~ 2 0
25 AGAL G001.692-00.171 DNe 17 50 15 -27 34.6           ~ 9 0
26 [M2012] G001.87-00.14 SMM 23 DNe 17 50 15.0 -27 21 33           ~ 3 0
27 [M2012] G001.87-00.14 SMM 28 smm 17 50 19.2067 -27 27 39.749           ~ 5 0
28 [M2012] G001.87-00.14 SMM 30 DNe 17 50 22.8 -27 21 28           ~ 2 0
29 [M2012] G001.87-00.14 SMM 31 smm 17 50 25.7108 -27 28 31.397           ~ 5 0
30 IRAS 17474-2704 IR 17 50 36.3 -27 05 43           ~ 11 0
31 AGAL G002.142+00.009 smm 17 50 36.9143 -27 05 50.321           ~ 11 0
32 [M2012] G001.87-00.14 SMM 38 DNe 17 50 46.8996 -27 24 37.223           ~ 5 0
33 [M2012] G011.36+00.80 SMM 1 smm 18 07 35.0 -18 43 46           ~ 2 0
34 [M2012] G011.36+00.80 SMM 3 smm 18 07 35.8 -18 42 42           ~ 2 0
35 SDC G11.360+0.800 DNe 18 07 35.98 -18 42 44.2           ~ 5 0
36 [M2012] G011.36+00.80 SMM 4 smm 18 07 36.1 -18 44 26           ~ 2 0
37 [M2012] G011.36+00.80 SMM 5 smm 18 07 36.7 -18 41 14           ~ 2 0
38 [M2012] G011.36+00.80 SMM 6 DNe 18 07 39.0 -18 42 10           ~ 2 0
39 SDC G11.361+0.777 DNe 18 07 41.23 -18 43 21.1           ~ 4 0
40 BGPS G013.123+00.066 smm 18 13 53.2158 -17 31 19.929           ~ 6 0
41 [M2012] G013.22-00.06 SMM 4 smm 18 13 55.9 -17 28 34           ~ 2 0
42 [WWS2012] G013.18+00.06 cor 18 14 01.2870 -17 28 33.276           ~ 11 1
43 [ABB2014] WISE G013.222+00.082 bub 18 14 01.3 -17 25 38           ~ 14 1
44 [ABB2014] WISE G013.186+00.042 bub 18 14 06.2 -17 28 31           ~ 25 0
45 [M2012] G013.22-00.06 SMM 6 smm 18 14 08.4761 -17 28 40.139           ~ 5 0
46 [M2012] G013.22-00.06 SMM 7 smm 18 14 09.4 -17 27 21           ~ 2 0
47 [ERG2015] 2855 cor 18 14 13.7292 -17 25 06.928           ~ 9 0
48 [M2012] G013.22-00.06 SMM 23 smm 18 14 36.8 -17 29 22           ~ 2 0
49 [M2012] G013.22-00.06 SMM 27 smm 18 14 40.7 -17 29 22           ~ 2 0
50 IRAS 18117-1738 IR 18 14 41.3 -17 37 04           ~ 9 0
51 [WWS2012] G013.13-00.15 cor 18 14 42.1731 -17 37 00.242           ~ 10 0
52 [WWS2012] G013.21-00.14 cor 18 14 50.009 -17 32 41.25           ~ 10 0
53 MSXDC G028.23-0.19 DNe 18 43 31.3 -04 13 18           ~ 26 0
54 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 94 0
55 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 505 0
56 MSXDC G035.39-0.33 MoC 18 57 09.0 +02 07 46           ~ 115 0
57 NAME K 3-50A HII 20 01 45.6 +33 32 42           ~ 80 0

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