2001MNRAS.326..805C


Query : 2001MNRAS.326..805C

2001MNRAS.326..805C - Mon. Not. R. Astron. Soc., 326, 805-820 (2001/September-2)

Maser emission from OH at the 6035-MHz transition.

CASWELL J.L.

Abstract (from CDS):

The Australia Telescope Compact Array (ATCA) has been used to measure positions with subarcsec accuracy for more than 50 masers at the 6035-MHz transition of excited OH. Eleven of the masers are new discoveries; the remainder complete the detailed study of masers from an earlier single-dish survey of the southern Galactic plane using the Parkes telescope. All previously known masers in the region were strong enough to be studied in the present observations, despite the common occurrence of variability. Typically, the intensity varies by less than a factor of two over several years, but one of the new masers is, remarkably, 100 times stronger than the upper limit measured six years earlier.

The precise positions confirm that most of the masers coincide with a 1665-MHz ground-state OH maser counterpart that is usually stronger. However, there are a few instances where any 1665-MHz counterpart is either much weaker or not detected. When surveyed with comparable sensitivity, we show that the 6035-MHz masers are approximately one-third as common as 1665-MHz masers. We also add to earlier evidence that 1720-MHz masers preferentially occur at the sites hosting 6035-MHz masers. These facts are discussed in the context of current maser pumping models.

Towards most of the 6035-MHz maser sites we find a coincident 6668-MHz methanol maser, and towards some of the maser sites we report new detections of ultracompact Hii regions. Clusters of two or three sites, each showing one, or several, of the principal molecular masing transitions, are found to be common; future comparative studies of these sites within small clusters will elucidate the precise conditions favouring different maser species. Several instances of absorption occur at 6035MHz, one of them especially striking since it extends over a broad velocity range adjacent to maser emission related to the ultracompact Hii region 5.885-0.392. The absorption provides new clues to understanding the geometry and excitation of 5.885-0.392.

Three sources were observed at 6030MHz, an OH transition from the same excited state (2Π3/2, J=5/2) as the 6035-MHz line; in one case, the matching velocity patterns at 6030 and 6035MHz, their similar circular polarization characteristics, and their spatial coincidence, reveal Zeeman splitting in a magnetic field of -9mG, a field strength close to the upper limit found for any such masers.


Abstract Copyright: The Royal Astronomical Society

Journal keyword(s): masers - stars: formation - Hii regions - ISM: molecules - radio lines: ISM

Nomenclature: Table 1: Caswell OH LLL.lll+BB.bbb N=53.

Simbad objects: 70

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Number of rows : 70
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 NAME W 3 OH HII 02 27 04.1 +61 52 22           ~ 1000 2
2 OH 348.698-00.027 Mas 09 58 59 -38 58.2           ~ 1 0
3 OH 306.32-00.36 Mas 13 21 23.01 -63 00 29.5           ~ 11 0
4 OH 309.92+00.48 Mas 13 50 41.78 -61 35 10.2           ~ 50 0
5 IRAS 14026-6145 * 14 06 18.459 -62 00 15.76           ~ 5 0
6 OH 316.76-00.01 Mas 14 44 56.34 -59 48 00.8           ~ 19 0
7 OH 319.39-00.02 Mas 15 03 17.41 -58 36 12.2           ~ 6 0
8 OH 328.24-00.55 Mas 15 57 58.28 -53 59 22.7           ~ 37 0
9 OH 329.339+00.148 Mas 16 00 33.15 -52 44 39.9           ~ 4 0
10 AGAL G329.066-00.307 HII 16 01 09.8 -53 16 01           ~ 37 0
11 OH 329.07-00.31 Y*O 16 01 09.999 -53 16 02.94           ~ 37 0
12 OH 329.405-00.459 Mas 16 03 32.16 -53 09 30.5           ~ 10 0
13 OH 330.9-00.2 OH* 16 09 35.53920 -51 54 14.1084           O-rich 12 0
14 Caswell H2O 331.51-00.10 Mas 16 12 09.1 -51 28 53           ~ 12 0
15 OH 332.826-00.549 Mas 16 20 10.85 -50 53 14.2           ~ 15 0
16 OH 336.36-00.14 Mas 16 33 29.17 -48 03 43.9           ~ 18 0
17 OH 336.83+00.02 Mas 16 34 38.28 -47 36 32.2           ~ 19 0
18 OH 336.941-00.156 Mas 16 35 55.19 -47 38 45.4           ~ 9 0
19 Caswell CH3OH 336.983-00.183 Mas 16 36 12.41 -47 37 58.2           ~ 24 0
20 IRAS 16325-4731 cor 16 36 12.41856 -47 37 57.8280           ~ 24 0
21 OH 337.40-00.41 Mas 16 38 50.52 -47 28 00.2           ~ 40 0
22 OH 338.08+00.01 Mas 16 39 39.04 -46 41 28.0           ~ 19 0
23 OH 338.92+00.55 Y*O 16 40 34.064 -45 42 08.68           ~ 18 0
24 MMB G339.282+00.136 Mas 16 43 43.11 -45 42 08.0           ~ 9 0
25 MMB G339.053-00.315 Mas 16 44 48.99 -46 10 13.0           ~ 10 0
26 OH 339.6-00.1 Y*O 16 46 05.99 -45 36 43.3           ~ 71 0
27 OH 339.88-01.26 Y*O 16 52 04.6776 -46 08 34.404           ~ 101 0
28 OH 344.39+00.03 Mas 17 02 08.62 -41 47 10.3           ~ 6 0
29 OH 344.58-00.02 Y*? 17 02 57.71 -41 41 53.8           ~ 39 0
30 OH 345.487+00.314 Mas 17 04 28.24 -40 46 28.7           ~ 12 0
31 OH 345.4-00.9 Mas 17 09 35.42 -41 35 57.1           ~ 31 0
32 OH 350.113+00.095 Mas 17 19 25.609 -37 10 05.38           ~ 17 0
33 OH 350.686-00.491 Mas 17 23 28.63 -37 01 48.8           ~ 11 0
34 OH 353.41-00.36 Mas 17 30 26.18 -34 41 45.6           ~ 65 0
35 MMB G000.666-00.029 Mas 17 47 18.64 -28 22 54.6           ~ 12 0
36 OH 000.658-00.042 Mas 17 47 20.485 -28 23 44.13           ~ 17 0
37 OH 003.910+00.001 Mas 17 54 38.75 -25 34 44.8           ~ 9 0
38 MMB G008.669-00.356 Mas 18 06 18.99 -21 37 32.2           ~ 37 0
39 OH 010.4+00.0 Mas 18 08 38.257 -19 51 49.04           ~ 32 0
40 OH 011.03+00.06 Mas 18 09 39.84 -19 21 20.3           ~ 31 0
41 OH 010.62-00.38 Mas 18 10 28.65 -19 55 49.5           ~ 28 0
42 OH 015.03-00.68 Mas 18 20 24.8111 -16 11 35.316           ~ 25 1
43 OH 019.48+00.15 Mas 18 26 00.39 -11 52 21.9           ~ 6 0
44 OH 020.23+00.07 Mas 18 27 44.56 -11 14 54.6           ~ 11 0
45 AGAL G022.434-00.169 cor 18 32 44.1639 -09 24 33.608           ~ 17 0
46 OH 028.201-00.049 Mas 18 42 58.197 -04 13 59.41           ~ 8 0
47 Caswell OH 028.86+00.07 Mas 18 43 48.1 -03 35 31           ~ 15 0
48 IRAS 18449-0115 cor 18 47 34.29 -01 12 44.5           ~ 370 0
49 GAL 032.15+00.13 Mas 18 49 32.2 -00 38 01           ~ 6 0
50 Caswell OH 032.74-00.08 Mas 18 51 21.8624 -00 12 06.220           ~ 11 0
51 OH 034.26+00.15 Mas 18 53 18.68 +01 15 00.3           ~ 31 0
52 Caswell OH 035.02+00.35 Mas 18 54 00.6576 +02 01 19.217           ~ 11 0
53 OH 035.2-00.7 Mas 18 58 13.0517 +01 40 35.674           ~ 40 0
54 OH 035.200-01.736 Mas 19 01 45.5420 +01 13 32.690           ~ 14 0
55 IRAS 19002+0654 Y*O 19 02 39.5357424288 +06 59 07.788621768           ~ 22 1
56 IRAS 19035+0641 Y*O 19 06 01.6288 +06 46 36.140           ~ 67 0
57 Caswell CH3OH 043.15+00.02 Mas 19 10 10.6 +09 05 27           ~ 3 0
58 OH 043.149+00.013 Mas 19 10 11.05 +09 05 22.1           ~ 2 0
59 Caswell CH3OH 043.16+00.02 Mas 19 10 11.9 +09 06 15           ~ 2 0
60 OH 043.165+00.013 Mas 19 10 13.034 +09 06 12.75           ~ 3 0
61 W 49n HII 19 10 13.2 +09 06 12           ~ 456 3
62 W 49 SFR 19 10 20 +09 07.7           ~ 557 1
63 NAME W 49A South HII 19 10 21.6 +09 05 03           ~ 53 2
64 OH 043.2+00.0 Y*O 19 10 21.819 +09 05 02.83           O2-3.5If* 27 0
65 OH 043.796-00.127 Mas 19 11 53.9868 +09 35 50.325           ~ 76 0
66 OH 045.122+00.133 Mas 19 13 27.942 +10 53 34.84           ~ 8 0
67 OH 045.466+00.045 Mas 19 14 25.66 +11 09 26.5           ~ 4 0
68 OH 049.489-00.388 Mas 19 23 43.8700 +14 30 29.500           ~ 4 0
69 OH 049.490-00.388 Mas 19 23 43.93 +14 30 34.9           ~ 4 0
70 W 51 SNR 19 23 50 +14 06.0           ~ 1249 1

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2023.06.04-16:55:32

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