Volume 549, January 2013
|Number of page(s)||22|
|Section||Interstellar and circumstellar matter|
|Published online||10 January 2013|
A double-jet system in the G31.41 + 0.31 hot molecular core⋆
INAF – Osservatorio Astrofisico di Arcetri, Largo E. Fermi 5,
e-mail: email@example.com; firstname.lastname@example.org
2 Purple Mountain Observatory, Chinese Academy of Sciences, 210008 Nanjing, PR China
e-mail: email@example.com; firstname.lastname@example.org
3 Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany
4 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA
Received: 4 October 2012
Accepted: 9 November 2012
Context. Many aspects of massive star (≳10 M⊙) formation are still unclear. In particular, the outflow properties at close distance (100–1000 AU) from a massive young stellar object (MYSO) are not yet well established.
Aims. This work presents a detailed study of the gas kinematics toward the hot molecular core (HMC) G31.41 + 0.31.
Methods. To study the HMC 3D kinematics at milli-arcsecond angular resolution, we performed multi-epoch VLBI observations of the H2O 22 GHz and CH3OH 6.7 GHz masers, and single-epoch VLBI of the OH 1.6 GHz masers.
Results. Water masers present a symmetric spatial distribution with respect to the HMC center, where two nearby (0".2 apart), compact, VLA sources (labeled “A” and “B”) are previously detected. The spatial distribution of a first group of water masers, named “J1”, is well fit with an elliptical profile, and the maser proper motions mainly diverge from the ellipse center, with average speed of 36 km s-1. These findings strongly suggest that the “J1” water maser group traces the heads of a young (dynamical time of 1.3 × 103 yr), powerful (momentum rate of ≃0.2 M⊙ yr-1 km s-1), collimated (semi-opening angle ≃10°) jet emerging from a MYSO located close (within ≈0".15) to the VLA source “B”. Most of the water features not belonging to “J1” present an elongated (≈2′′ in size), NE-SW oriented (PA ≈ 70°), S-shape distribution, which we denote with the label “J2”. The elongated distribution of the “J2” group and the direction of motion, approximately parallel to the direction of elongation, of most “J2” water masers suggests the presence of another collimated outflow, emitted from a MYSO placed near the VLA source “A”. The proper motions of the CH3OH 6.7 GHz masers, mostly diverging from the HMC center, also witness the expansion of the HMC gas driven by the “J1” and “J2” jets. The orientation (PA ≈ 70°) of the “J2” jet agrees well with that (PA = 68°) of the well-defined VLSR gradient across the HMC revealed by previous interferometric, thermal line observations. Furthermore, the “J2” jet is powerful enough to sustain the large momentum rate, 0.3 M⊙ yr-1 km s-1, estimated from the interferometric, molecular line data in the assumption that the VLSR gradient represents a collimated outflow. These two facts lead us to favor the interpretation of the VLSR gradient across the G31.41 + 0.31 HMC in terms of a compact and collimated outflow.
Key words: techniques: interferometric / masers / ISM: kinematics and dynamics
Tables 2–5 are available in electronic form at http://www.aanda.org
© ESO, 2013
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