Abstract
Abstract We present high-resolution observations of CS (J = 1–0), H13CO+ (J = 1–0), and SiO (v = 0: J = 1–0) lines, together with the 49 GHz and 86 GHz continuum emissions, toward W 49 N carried out with the Nobeyama Millimeter Array. We identified 11 CS, eight H13CO+, and six SiO clumps with radii of 0.1–0.5 pc. The CS and H13CO+ clumps are mainly divided into two velocity components, one at 4 km s−1 and the other at 12 km s−1, while the SiO clumps have velocities between the two components. The SiO emission is distributed toward the ultracompact H ii (UCHII) ring, where the 4 km s−1 component clumps of CS and H13CO+ also exist. The 12 km s−1 component clumps of CS are detected at the east and west of the UCHII ring with an apparent hole toward the ring. The clump masses vary from 4.4 × 102 M$_\odot$ to 4.9 × 104 M$_\odot$ with the mean values of 0.94 × 104 M$_\odot$, 0.88 × 104 M$_\odot$, and 2.2 × 104 M$_\odot$ for the CS, H13CO+, and SiO clumps, respectively. The total masses derived from CS, H13CO+, and SiO clumps are 1.0 × 105 M$_\odot$, 0.70 × 105 M$_\odot$, and 1.3 × 105 M$_\odot$, respectively, which agree well with the corresponding virial masses of 0.71 × 105 M$_\odot$, 1.3 × 105 M$_\odot$, and 0.88 × 105 M$_\odot$, respectively. The average molecular hydrogen densities of the clumps are 0.90 × 106 cm−3, 1.4 × 106 cm−3, and 7.6 × 106 cm−3 for the CS, H13CO+, and SiO clumps, respectively. The density derived from the SiO clumps seems significantly higher than those from the others, probably because the SiO emission is produced in high-density shocked regions. The free-fall time scale of the clumps is estimated to be ∼3 × 104 yr, which gives an accretion rate of 3 × 10−3–1 M$_\odot$ yr−1 on to a stellar core. The observed clumps are, if they are undergoing free-fall, capable of producing dozens of massive stars in the next 105 yr. We propose a view that two pre-existing clouds with radial velocities of 4 km s−1 and 12 km s−1 collided with each other almost face-on to produce the observed clumps with intermediate velocities and triggered the burst of massive star formation in W 49 N.
Highlights
The thermal radio source W49A is one of the most luminous HII region/molecular cloud complexes in our Galaxy located at a distance of 11.11+−00..7699 kpc (Zhang et al 2013)
We propose a view that pre-existing two clouds having the radial velocities of 4 km s−1 and 12 km s−1 collided with each other almost face-on to produce the observed clumps with intermediate velocities and triggered the burst of massive star formation in W49N
In this paper we present Nobeyama Millimeter Array (NMA) observations of the massive molecular cloud core W49N with the transitions of CS (J = 1 – 0), SiO (J = 2 – 1), and H13CO+ (J = 1 – 0) together with the 49 GHz and 86 GHz continuum emissions
Summary
The thermal radio source W49A is one of the most luminous HII region/molecular cloud complexes in our Galaxy located at a distance of 11.11+−00..7699 kpc (Zhang et al 2013). High resolution continuum observations of W49N at centimeter and millimeter wavelengths have revealed clusters of Publications of the Astronomical Society of Japan, (2021), Vol 00, No 0 ultra-compact HII regions (UCHII ring) located along an ellipse, or a tilted ring, with a diameter of 1.5 pc (∼ 25 ) (Welch et al 1987). The source G, which in itself consists of at least several UCHII regions (e.g., Dreher et al 1984; De Pree et al 1997), is the brightest among them. It is the most luminous H2O maser source in the Galaxy (e.g., Walker et al 1982)
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