2018A&A...609A.125W


Query : 2018A&A...609A.125W

2018A&A...609A.125W - Astronomy and Astrophysics, volume 609A125-125 (2018/1-1)

ATLASGAL - Ammonia observations towards the southern Galactic plane.

WIENEN M., WYROWSKI F., MENTEN K.M., URQUHART J.S., WALMSLEY C.M., CSENGERI T., KORIBALSKI B.S. and SCHULLER F.

Abstract (from CDS):

Context. The initial conditions of molecular clumps in which high-mass stars form are poorly understood. In particular, a more detailed study of the earliest evolutionary phases is needed. The APEX Telescope Large Area Survey of the whole inner Galactic disk at 870 µm, ATLASGAL, has therefore been conducted to discover high-mass star-forming regions at different evolutionary phases.
Aims. We derive properties such as velocities, rotational temperatures, column densities, and abundances of a large sample of southern ATLASGAL clumps in the fourth quadrant.
Methods. Using the Parkes telescope, we observed the NH3 (1,1) to (3,3) inversion transitions towards 354 dust clumps detected by ATLASGAL within a Galactic longitude range between 300° and 359° and a latitude within±1.5°. For a subsample of 289 sources, the N2H+ (1-0) line was measured with the Mopra telescope.
Results. We measured a median NH3 (1,1) line width of ∼2km/s, rotational temperatures from 12 to 28K with a mean of 18K, and source-averaged NH3 abundances from 1.6x10–6 to 10–8. For a subsample with detected NH3 (2,2) hyperfine components, we found that the commonly used method to compute the (2,2) optical depth from the (1,1) optical depth and the (2,2) to (1,1) main beam brightness temperature ratio leads to an underestimation of the rotational temperature and column density. A larger median virial parameter of ∼1 is determined using the broader N2H+ line width than is estimated from the NH3 line width of ∼0.5 with a general trend of a decreasing virial parameter with increasing gas mass. We obtain a rising NH3 (1,1)/N2H+ line-width ratio with increasing rotational temperature.
Conclusions. A comparison of NH3 line parameters of ATLASGAL clumps to cores in nearby molecular clouds reveals smaller velocity dispersions in low-mass than high-mass star-forming regions and a warmer surrounding of ATLASGAL clumps than the surrounding of low-mass cores. The NH3 (1,1) inversion transition of 49% of the sources shows hyperfine structure anomalies. The intensity ratio of the outer hyperfine structure lines with a median of 1.27±0.03 and a standard deviation of 0.45 is significantly higher than 1, while the intensity ratios of the inner satellites with a median of 0.9±0.02 and standard deviation of 0.3 and the sum of the inner and outer hyperfine components with a median of 1.06±0.02 and standard deviation of 0.37 are closer to 1.

Abstract Copyright: © ESO, 2018

Journal keyword(s): submillimeter: ISM - surveys - ISM: molecules - ISM: kinematics and dynamics - stars: formation - stars: massive

Simbad objects: 39

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Number of rows : 39
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 1448 DNe 03 22.5 +30 35           ~ 546 0
2 LDN 1455 DNe 03 28 00.6480 +30 07 58.800           ~ 198 1
3 NGC 1333 OpC 03 29 09.2 +31 20 59           ~ 1575 1
4 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1553 0
5 IC 348 OpC 03 44 31.1 +32 10 02           ~ 1476 1
6 NAME Gemini OB1 Molecular Cloud MoC 06 19.0 +23 00           ~ 49 0
7 IRAS 12326-6245 HII 12 35 35.184 -63 02 29.40           ~ 55 0
8 AGAL G305.369+00.166 Y*O 13 12 38.858 -62 36 22.46           ~ 8 0
9 NAME G305 Complex SFR 13 13 -62.7           ~ 72 0
10 AGAL G326.641+00.612 smm 15 44 33.490 -54 05 31.00           ~ 19 0
11 OH 327.3-00.6 Mas 15 53 07.65 -54 37 06.1           ~ 35 1
12 SDC G328.277-0.551 DNe 15 58 12.05 -53 58 00.7           ~ 3 0
13 Caswell H2O 331.51-00.10 Mas 16 12 09.1 -51 28 53           ~ 12 0
14 AGAL G333.018+00.766 smm 16 15 18 -49 48.7           ~ 17 0
15 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
16 AGAL G336.824+00.027 smm 16 34 38.350 -47 36 30.38           ~ 17 0
17 AGAL G343.501+00.026 Y*O 16 59 10 -42 31.2           ~ 16 0
18 AGAL G345.258-00.036 cor 17 05 12.197 -41 10 07.92           ~ 13 0
19 GAL 347.6+00.2 HII 17 11 33.8 -39 08 20           ~ 22 0
20 AGAL G348.549-00.979 smm 17 19 20 -39 03.9           ~ 18 0
21 AGAL G350.102+00.082 cor 17 19 27.2 -37 11 02           ~ 18 0
22 AGAL G351.141+00.776 Y*O 17 19 35.7 -35 56 05           ~ 12 0
23 AGAL G348.759-00.946 Y*O 17 19 49.010 -38 52 27.26           ~ 14 0
24 NGC 6334 HII 17 20 53 -36 07.9           ~ 740 0
25 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 373 0
26 AGAL G351.456+00.666 Y*O 17 20 55 -35 44.4           ~ 9 0
27 NAME the Pipe Nebula DNe 17 30 -25.0           ~ 442 1
28 AGAL G354.616+00.472 smm 17 30 16.990 -33 13 57.38           ~ 16 0
29 AGAL G354.748+00.369 Y*O 17 31 03 -33 10.6           ~ 11 0
30 IRAS 17279-3311 Y*? 17 31 15.5976886344 -33 14 04.872124932           ~ 37 0
31 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 380 0
32 NGC 6618 OpC 18 20 47 -16 10.3           ~ 1700 0
33 MMB G015.665-00.499 Y*? 18 20 59.7470 -15 33 09.800           ~ 29 0
34 SDC G23.330-0.295 DNe 18 34 51.36 -08 40 23.9           ~ 11 0
35 CORNISH G030.7197-00.0829 Y*O 18 47 41.79 -02 00 22.3           ~ 24 0
36 GAL 035.03+00.35 cor 18 54 00.60 +02 01 19.3           ~ 48 0
37 IRAS 20126+4104 Y*O 20 14 25.8816769656 +41 13 36.879427236           B2.5-B0.5 469 0
38 DR 21 (OH) cor 20 39 01.01 +42 22 50.2           ~ 427 0
39 NAME Galactic Bar reg ~ ~           ~ 1458 0

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