2005AJ....129..330W


Query : 2005AJ....129..330W

2005AJ....129..330W - Astron. J., 129, 330-347 (2005/January-0)

CO J = 2-1 maps of bipolar outflows in massive star-forming regions.

WU Y., ZHANG Q., CHEN H., YANG C., WEI Y. and HO P.T.P.

Abstract (from CDS):

Using the eight-beam array receiver of the NRAO 12 m telescope, we mapped the CO J=2-1 emission toward 11 high-mass star-forming regions. In the sample, four are previously detected outflows in the CO J=1-0 line, and seven are outflow candidates. A total of six bipolar outflows were identified in the CO J=2-1 line. For the remaining five sources, including one previously detected bipolar outflow, the CO J=2-1 emission shows multiple velocity components. Therefore, high-velocity line wings or bipolar structure cannot be identified. The CO J=2-1 spectra of the four of the nonbipolar outflow sources exhibit broad-line emission due to the blending of weak velocity components. The complex CO spectra underscore the importance of large-scale mapping in identifying outflows. Compared with the outflows detected with the CO J=1-0 line, the CO J=2-1 outflows often have broader line wings and smaller spatial extents, indicating that the high-velocity gas measured with the CO J=2-1 line arises from warm regions closer to the central source. The masses in the outflows range from a few to 60 M. The linear momenta in the outflows are as large as a few hundred Mkm/s. Both parameters are much larger than the typical values in low-mass outflows. The average dynamic timescale of the outflows is 2x104 yr. The driving sources of the bipolar outflows are also identified. All bipolar outflows detected have a near-infrared source, except for IRAS 23385+6053, and all are associated with centimeter or millimeter continuum emission, except for IRAS 22506+5549. We investigated the correlation between the outflow parameters and the properties of the driving source. The outflow luminosity and mechanical force correlate with the bolometric luminosity of the star. However, the mechanical force required to drive a CO outflow is more than an order of magnitude higher than the radiation pressure from the star. We reexamined the relation between the mass entrainment rate of the outflows and the bolometric luminosity of the central source with an up-to-date sample.
Result. show that the mass outflow rate increases with increasing bolometric luminosity, suggesting that the mass outflow rate is related to the luminosity of the central source.

Abstract Copyright:

Journal keyword(s): ISM: Jets and Outflows - ISM: Kinematics and Dynamics - ISM: Molecules - ISM: Masers - Stars: Formation

CDS comments: In abstract : IRAS 22506+5549 is a misprint for IRAS 22506+5944. In table 2 : IRAS 22543+6154 is a misprint for IRAS 22543+6145. Source S4 is 2MASS J22523871+6000445 in Simbad.

Simbad objects: 24

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Number of rows : 24
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* V415 Ori Or* 05 35 21.8787666816 -05 07 01.837785036     14.49   12.64 ~ 50 0
2 OMC 2 MoC 05 35 27 -05 10.1           ~ 449 1
3 NAME OMC 2 IRS 4 IR 05 35 27.3 -05 09 39           ~ 18 0
4 2MASS J05352762-0509337 Y*O 05 35 27.622 -05 09 33.78           ~ 96 0
5 V* V2467 Ori Or* 05 35 27.6431954136 -05 09 37.148090580         19.580 ~ 44 0
6 V* V419 Ori TT* 05 35 28.1499634584 -05 10 13.874935764     15.46   12.95 M2e 60 0
7 NAME HH 80-81 IRS HII 18 19 11.8 -20 47 35           ~ 148 0
8 [KCW94] 010.841-02.592 Rad 18 19 12.098 -20 47 30.90           ~ 6 0
9 2MASS J18191220-2047297 Y*O 18 19 12.21 -20 47 29.7           B1 133 0
10 IRAS 18314-0720 HII 18 34 09.3 -07 18 00           ~ 31 0
11 IRAS 18556+0139 mul 18 58 11.5 +01 43 53           ~ 2 0
12 GAL 035.2-00.74 cor 18 58 13.00 +01 40 36.0           ~ 169 0
13 IRAS 18556+0136 mul 18 58 13.1 +01 40 35           ~ 139 0
14 IRAS 19209+1421 IR 19 23 12.3 +14 26 52           ~ 13 0
15 IRAS 19209+1418 IR 19 23 15.5 +14 24 19           ~ 2 0
16 BG 2247+59 LP? 22 49 29.0034646608 +59 54 56.182749876           ~ 107 1
17 IRAS 22506+5944 Y*O 22 52 38.09760 +60 01 01.1928           ~ 58 0
18 2MASS J22523871+6000445 Y*O 22 52 38.71 +60 00 44.5           ~ 4 0
19 GAL 109.88+02.11 HII 22 56 19.4 +62 02 01           ~ 74 0
20 2MASS J22561976+6201509 NIR 22 56 19.77 +62 01 51.0           ~ 1 0
21 IRAS 23042+6000 IR 23 06 22.2177213936 +60 16 17.842393560           ~ 19 0
22 SH 2-159 Y*O 23 15 31.2384366062 +61 07 10.181362705           ~ 180 2
23 2MASS J23405396+6110421 NIR 23 40 53.96 +61 10 42.1           ~ 1 0
24 Mol 160 Rad 23 40 54.5 +61 10 28           ~ 104 0

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