2010A&A...509A..50C


Query : 2010A&A...509A..50C

2010A&A...509A..50C - Astronomy and Astrophysics, volume 509, A50-50 (2010/1-1)

The structure of hot molecular cores over 1000 AU.

CESARONI R., HOFNER P., ARAYA E. and KURTZ S.

Abstract (from CDS):

Hot molecular cores (HMCs) are believed to be the cradles of stars of mass above ∼6M. It is hence important to determine their structure and kinematics and thus study phenomena directly related to the star-formation process, such as outflow, infall, and rotation. Establishing the presence of embedded early-type (proto)stars is also crucial for understanding the nature of HMCs. To achieve the highest available angular resolution to date, we performed observations of the molecular gas in two well-known HMCs (G10.47+0.03 and G31.41+0.31) with an angular resolution of ∼0.1". Continuum observations were also made at different wavelengths to detect Hii regions associated with early-type stars embedded in the cores. We used the Very Large Array in its most extended configuration to image the NH3(4,4) inversion transition. Continuum measurements were made at 7 mm, 1.3cm, and 3.6cm using the A-array configuration. We detected two new continuum sources in G31.41+0.31, which are possibly thermal jets, and confirmed the presence of one ultracompact and two hypercompact HII regions in G10.47+0.03. Evidence that the gas is infalling towards the embedded (proto)stars is provided for both G10.47+0.03 and G31.41+0.31, while in G10.47+0.03 part of the ammonia gas also appears to be expanding in two collimated bipolar outflows. From the temperature profile in the cores, we establish an approximate bolometric luminosity for both sources in the range 1x105-7x105L. Finally, a clear velocity gradient across the core is detected in G31.41+0.31. The nature of this gradient is discussed and two alternative explanations are proposed: outflow and rotation. We propose a scenario where G10.47+0.03 is in a more advanced evolutionary stage than G31.41+0.31. In this scenario, thermal jets develop until the accretion rate is sufficiently high to trap or even quench any HII region. When the jets have pierced the core and the stellar mass has grown sufficiently, hypercompact HII regions appear and the destruction of the HMC begins.

Abstract Copyright:

Journal keyword(s): stars: formation - HII regions - ISM: individual objects: G10.47+0.03, G31.41+0.31 - ISM: molecules

Nomenclature: Table 2: [WC89] LLL.ll+B.bbA (No. 10.47+0.03D) added. Table 3: [WC89] LLL.ll+B.bbA (Nos 031.41+0.31A-B) added.

Simbad objects: 13

goto Full paper

goto View the references in ADS

Number of rows : 13
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 Orion Core ? 05 35 14.5 -05 22 30           ~ 195 0
2 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4189 2
3 QSO B1730-130 QSO 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1093 1
4 PMN J1755-2232 Rad 17 55 26.284538 -22 32 10.61562           ~ 32 0
5 [GRM93] G10.46+0.03 A HII 18 08 38.19 -19 51 49.4           ~ 10 0
6 [WC89] 010.47+0.03B2 HII 18 08 38.22 -19 51 50.5           ~ 7 0
7 [WC89] 010.47+0.03B1 HII 18 08 38.25 -19 51 50.1           ~ 8 0
8 [WC89] 010.47+0.03D HII 18 08 38.274 -19 51 48.09           ~ 1 0
9 GAL 010.47+00.03 HII 18 08 38.4 -19 51 52           ~ 134 0
10 QSO J1820-2528 QSO 18 20 57.84869964 -25 28 12.5840414   18.56       ~ 93 0
11 IRAS 18449-0115 cor 18 47 34.29 -01 12 44.5           ~ 369 0
12 NVSS J185146+003532 Rad 18 51 46.72295 +00 35 32.3649           ~ 66 1
13 PSR B1849+00 Psr 18 52 27.42 +00 32 02.0           ~ 68 0

To bookmark this query, right click on this link: simbad:objects in 2010A&A...509A..50C and select 'bookmark this link' or equivalent in the popup menu


2023.03.26-14:40:46

© Université de Strasbourg/CNRS

    • Contact