2021A&A...645A..29K


Query : 2021A&A...645A..29K

2021A&A...645A..29K - Astronomy and Astrophysics, volume 645A, 29-29 (2021/1-1)

Search for radio jets from massive young stellar objects. Association of radio jets with H2O and CH3OH masers.

KAVAK U., SANCHEZ-MONGE A., LOPEZ-SEPULCRE A., CESARONI R., VAN DER TAK F.F.S., MOSCADELLI L., BELTRAN M.T. and SCHILKE P.

Abstract (from CDS):


Context. Recent theoretical and observational studies debate the similarities of the formation process of high- (>8M) and low-mass stars. The formation of low-mass stars is directly associated with the presence of disks and jets. Theoretical models predict that stars with masses up to 140M can be formed through disk-mediated accretion in disk-jet systems. According to this scenario, radio jets are expected to be common in high-mass star-forming regions.
Aims. We aim to increase the number of known radio jets in high-mass star-forming regions by searching for radio-jet candidates at radio continuum wavelengths.
Methods. We used the Karl G. Jansky Very Large Array (VLA) to observe 18 high-mass star-forming regions in the C band (6cm, ≃1.0" resolution) and K band (1.3cm, ≃0.3" resolution). We searched for radio-jet candidates by studying the association of radio continuum sources with shock activity signs (e.g., molecular outflows, extended green objects, and maser emission). Our VLA observations also targeted the 22GHz H2O and 6.7GHz CH3OH maser lines.
Results. We have identified 146 radio continuum sources, 40 of which are located within the field of view of both images (C and K band maps). We derived the spectral index, which is consistent with thermal emission (between -0.1 and +2.0) for 73% of these sources. Based on the association with shock-activity signs, we identified 28 radio-jet candidates. Out of these, we identified 7 as the most probable radio jets. The radio luminosity of the radio-jet candidates is correlated with the bolometric luminosity and the outflow momentum rate. About 7-36% of the radio-jet candidates are associated with nonthermal emission. The radio-jet candidates associated with 6.7GHz CH3OH maser emission are preferentially thermal winds and jets, while a considerable fraction of radio-jet candidates associated with H2O masers show nonthermal emission that is likely due to strong shocks.
Conclusions. About 60% of the radio continuum sources detected within the field of view of our VLA images are potential radio jets. The remaining sources could be compact HII regions in their early stages of development, or radio jets for which we currently lack further evidence of shock activity. Our sample of 18 regions is divided into 8 less evolved infrared-dark regions and 10 more evolved infrared-bright regions. We found that ≃71% of the identified radio-jet candidates are located in the more evolved regions. Similarly, 25% of the less evolved regions harbor one of the most probable radio jets, while up to 50% of the more evolved regions contain one of these radio-jet candidates. This suggests that the detection of radio jets in high-mass star-forming regions is more likely in slightly more evolved regions.

Abstract Copyright: © ESO 2020

Journal keyword(s): stars: formation - stars: massive - ISM: jets and outflows - radio continuum: ISM - HII regions

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 42

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Number of rows : 42
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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2815 2
2 IRAS 05358+3543 Y*O 05 39 09.92 +35 45 17.2           ~ 164 0
3 7C 055201.39+394824.00 Bla 05 55 30.80561419 +39 48 49.1649683     18.30 17.5   ~ 505 2
4 NVSS J055932+235354 Rad 05 59 32.03313313 +23 53 53.9267334           ~ 49 1
5 JCMTSF J060835.2+203902 Mas 06 08 35.4 +20 39 03           ~ 7 0
6 GAL 192.58-00.04 HII 06 12 53.16 +18 00 23.3           ~ 25 0
7 [HBM2005] G192.60-0.05 mm 06 12 54.0 +17 59 23           ~ 4 0
8 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
9 IRAS 16547-4247 Y*O 16 58 17.208 -42 52 08.16           ~ 161 0
10 IRAS 16562-3959 SFR 16 59 42.257 -40 03 45.17           ~ 67 0
11 NAME HH 80-81 HH 18 19 06 -20 51.4           ~ 224 0
12 [CBH2011c] F G18.67+0.03 -CM1 Rad 18 24 52.6056 -12 39 20.005           ~ 3 0
13 [WWS2012] G018.17-00.30 cor 18 25 07 -13 14.5           ~ 16 0
14 IRAS 18223-1243 Y*O 18 25 10.9307288448 -12 42 15.754722912           ~ 61 1
15 IRAS 18228-1312 HII 18 25 42.2 -13 10 20           ~ 40 1
16 AGAL G019.286+00.082 Y*O 18 25 52.11528 -12 04 49.8900           ~ 28 0
17 [CCE98b] 019.30+0.07 Cld 18 25 56.78 -12 04 25.0           ~ 13 0
18 [PWC2006] NH3 G19.30+0.07 P1 cor 18 25 58.5 -12 03 59           ~ 7 0
19 GAL 019.36-00.02 HII 18 26 24.3 -12 03 47           ~ 31 0
20 [LZL2014] IRAS 18236-1205 P8 cor 18 26 25.610 -12 04 23.60           ~ 2 0
21 GAL 019.36-00.03 HII 18 26 25.80 -12 03 57.0           ~ 2 0
22 [CBH2011c] F G19.36-0.03 -CM2 Rad 18 26 26.379 -12 04 19.90           ~ 2 0
23 ICRF J183220.8-103511 G 18 32 20.83647 -10 35 11.1968           ~ 103 1
24 [RJS2006] MSXDC G023.60+00.00 MM1 mm 18 34 11.6 -08 19 06           ~ 14 0
25 RAFGL 7009S HII 18 34 20.911 -05 59 42.23           ~ 214 0
26 [RJS2006] MSXDC G024.08+00.04 MM2 mm 18 34 51.1 -07 45 32           ~ 9 0
27 HIGALBM G024.1835+00.1205 smm 18 34 57.0 -07 43 26           ~ 7 0
28 IRAS 18324-0737 mm 18 35 08.1 -07 35 04           ~ 22 0
29 AGAL G024.629+00.172 Y*O 18 35 35.6 -07 18 12           ~ 37 0
30 EGO G024.63+0.15 of? 18 35 40.1 -07 18 35           ~ 8 0
31 [RSJ2007] G024.60+00.08 MM1 B PoC 18 35 40.12 -07 18 36.9           ~ 2 0
32 [RSJ2007] G024.60+00.08 MM1 A PoC 18 35 40.12 -07 18 35.3           ~ 2 0
33 [RSJ2007] G024.60+00.08 MM1 C PoC 18 35 40.20 -07 18 37.2           ~ 2 0
34 [RJS2006] MSXDC G024.60+00.08 MM1 mm 18 35 40.2 -07 18 37           ~ 15 0
35 NVSS J185146+003532 Rad 18 51 46.72295 +00 35 32.3649           ~ 84 1
36 EGO G034.41+0.24 of? 18 53 17.9 +01 25 25           ~ 15 0
37 AGAL G034.411+00.234 Y*O 18 53 18.0319 +01 25 25.500           ~ 94 0
38 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 505 0
39 AGAL G034.459+00.247 Y*O 18 53 20.4 +01 28 23           ~ 67 0
40 [DLW84] G35.2N HII 18 58 13.036 +01 40 36.00           ~ 116 0
41 IRAS 19095+0930 cor 19 11 54.09216 +09 35 49.6896           ~ 101 0
42 NAME Cep A HW 2 Y*O 22 56 17.9 +62 01 49           B0.5 227 0

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