2020A&A...635A.118M


Query : 2020A&A...635A.118M

2020A&A...635A.118M - Astronomy and Astrophysics, volume 635A, 118-118 (2020/3-1)

Protostellar Outflows at the EarliesT Stages (POETS). IV. Statistical properties of the 22 GHz H2O masers.

MOSCADELLI L., SANNA A., GODDI C., KRISHNAN V., MASSI F. and BACCIOTTI F.

Abstract (from CDS):


Context. 22GHz water masers are the most intense and widespread masers in star-forming regions. They are commonly associated with protostellar winds and jets emerging from low- and high-mass young stellar objects (YSO).
Aims. We wish to perform for the first time a statistical study of the location and motion of individual water maser cloudlets, characterized by typical sizes that are within a few au, with respect to the weak radio thermal emission from YSOs.
Methods. For this purpose, we have been carrying out the Protostellar Outflows at the EarliesT Stages survey of a sample (38) of high-mass YSOs. The 22GHz water maser positions and three-dimensional (3D) velocities were determined through multi-epoch Very Long Baseline Array observations with accuracies of a few milliarcsec (mas) and a few km/s, respectively. The position of the ionized core of the protostellar wind, marking the YSO, was determined through sensitive radio continuum, multi-frequency Jansky Very Large Array observations with a typical error of ~=20 mas.
Results. The statistic of the separation of the water masers from the radio continuum shows that 84% of the masers are found within 1000au from the YSO and 45% of them are within 200au. Therefore, we can conclude that the 22GHz water masers are a reliable proxy for locating the position of the YSO. The distribution of maser luminosity is strongly peaked towards low values, indicating that about half of the maser population is still undetected with the current Very Long Baseline Interferometry detection thresholds of 50-100mJy/beam. Next-generation, sensitive (at the nJy level) radio interferometers will have the capability to exploit these weak masers for an improved sampling of the velocity and magnetic fields around the YSOs. The average direction of the water maser proper motions provides a statistically-significant estimate for the orientation of the jet emitted by the YSO: 55% of the maser proper motions are directed on the sky within an angle of 30° from the jet axis. Finally, we show that our measurements of 3D maser velocities statistically support models in which water maser emission arises from planar shocks with propagation direction close to the plane of the sky.

Abstract Copyright: © ESO 2020

Journal keyword(s): ISM: jets and outflows - ISM: molecules - masers - radio continuum: ISM - techniques: interferometric

Simbad objects: 34

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Number of rows : 34
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 IRAS 04579+4703 Y*O 05 01 39.661 +47 07 21.92           ~ 50 0
2 MSX6C G168.0627+00.8221 Y*O 05 17 13.8 +39 22 20           ~ 3 0
3 GAL 174.20-00.08 Cld 05 30 45.9 +33 47 56           ~ 205 2
4 [HLB98] Onsala 52 Mas 05 39 28.2 +24 56 32           ~ 2 0
5 MSX6C G229.5711+00.1525 Mas 07 23 01.7718 -14 41 34.339           ~ 8 0
6 IRAS 07422-2001 HII 07 44 28.2367 -20 08 30.606           ~ 23 0
7 [HLB98] SEST 26 Mas 07 44 51.9676 -24 07 42.372           ~ 5 0
8 OH 359.970-00.457 Mas 17 47 20.17 -29 11 59.4           ~ 7 0
9 OH 005.90-00.38 Mas 18 00 30.373 -24 04 00.96           ~ 46 1
10 MMB G009.986-00.028 cor 18 07 50.12 -20 18 56.5           ~ 25 0
11 OH 012.68-00.18 Mas 18 13 54.7457 -18 01 46.588           ~ 46 0
12 [HC96] G11.94-0.62 1 Mas 18 13 58.1205 -18 54 20.278           ~ 7 0
13 GAL 012.90-00.24 Mas 18 14 34.4366 -17 51 51.891           ~ 7 0
14 GAL 012.43-01.12 Mas 18 16 52.5 -18 41 50           ~ 6 0
15 GAL 014.63-00.58 Mas 18 19 14.7 -16 30 06           ~ 7 0
16 OH 016.59-00.05 Mas 18 21 09.0840 -14 31 48.556           ~ 81 0
17 RAFGL 5502 SFR 18 33 30.399 -05 01 02.73           ~ 24 0
18 AGAL G031.581+00.077 cor 18 48 42 -01 10.0           ~ 24 1
19 EGO G035.03+0.35 of? 18 54 00.5 +02 01 18           ~ 32 0
20 W 49n HII 19 10 13.2 +09 06 12           ~ 469 3
21 AGAL G049.189-00.336 Y*O 19 22 57 +14 16.1           ~ 8 0
22 IRAS 20126+4104 Y*O 20 14 25.8816769656 +41 13 36.879427236           B2.5-B0.5 440 0
23 GAL 075.76+00.34 Mas 20 21 41.0860 +37 25 29.280           ~ 22 1
24 GAL 075.78+00.34 cor 20 21 44.00 +37 26 38.0           ~ 126 1
25 GAL 074.03-01.71 Mas 20 25 07.1053 +34 49 57.593           ~ 6 0
26 [BE83] Maser 076.36-00.60 Mas 20 27 25.7 +37 22 52           ~ 5 0
27 [HLB98] Onsala 148 Mas 21 02 22.8 +50 03 07           ~ 4 0
28 [HLB98] Onsala 150 Mas 21 09 21.7320 +52 22 37.080           ~ 5 0
29 NAME S128(H20) Mas 21 32 11.44 +55 53 54.7           ~ 18 0
30 GAL 105.42+09.88 ? 21 43 06.67 +66 07 04.1           ~ 3 0
31 GAL 100.38-03.58 Mas 22 16 10.21 +52 21 32.1           ~ 4 0
32 2MASS J22493142+5955421 Y*O 22 49 31.4775 +59 55 42.006           ~ 11 0
33 IRAS 23139+5939 Y*O 23 16 10.3420 +59 55 28.596           ~ 97 0
34 MSX6C G111.2348-01.2385 Y*O 23 17 20.7888 +59 28 46.970           ~ 13 0

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