14 research outputs found
Molecular Clouds in the Galactic Plane from = [59.75, 74.75] and = [5.25, +5.25]
In this paper we present the distribution of molecular gas in the Milky Way
Galactic plane from = [59.75, 74.75] and = [5.25,
+5.25], using the MWISP CO/CO/
emission line data. The molecular gas in this region can be mainly attributed
to the Local spur, Local arm, Perseus arm, and Outer arm. Statistics of the
physical properties of the molecular gas in each arm, such as excitation
temperature, optical depth, and column density, are presented. Using the DBSCAN
algorithm, we identified 15 extremely distant molecular clouds with kinematic
distances of 14.7217.77 kpc and masses of 363520 M, which we
find could be part of the Outer Scutum-Centaurus (OSC) arm identified by
\cite{2011ApJ...734L..24D} and \cite{2015ApJ...798L..27S}. It is also possible
that, 12 of these 15 extremely distant molecular clouds constitute an
independent structure between the Outer and the OSC arms or a spur. There exist
two Gaussian components in the vertical distribution of the molecular gas in
the Perseus spiral arm. These two Gaussian components correspond to two giant
filaments parallel to the Galactic plane. We find an upward warping of the
molecular gas in the Outer spiral arm with a displacement of around 270 pc with
respect to the Galactic mid-plane.Comment: 33 pages, 19 figure
Carbon-Chain Molecules in Molecular Outflows and Lupus I Region--New Producing Region and New Forming Mechanism
Using the new equipment of the Shanghai Tian Ma Radio Telescope, we have
searched for carbon-chain molecules (CCMs) towards five outflow sources and six
Lupus I starless dust cores, including one region known to be characterized by
warm carbon-chain chemistry (WCCC), Lupus I-1 (IRAS 15398-3359), and one TMC-1
like cloud, Lupus I-6 (Lupus-1A). Lines of HC3N J=2-1, HC5N J=6-5, HC7N
J=14-13, 15-14, 16-15 and C3S J=3-2 were detected in all the targets except in
the outflow source L1660 and the starless dust core Lupus I-3/4. The column
densities of nitrogen-bearing species range from 10 to 10
cm and those of CS are about 10 cm. Two outflow
sources, I20582+7724 and L1221, could be identified as new
carbon-chain--producing regions. Four of the Lupus I dust cores are newly
identified as early quiescent and dark carbon-chain--producing regions similar
to Lup I-6, which together with the WCCC source, Lup I-1, indicate that
carbon-chain-producing regions are popular in Lupus I which can be regard as a
Taurus like molecular cloud complex in our Galaxy. The column densities of C3S
are larger than those of HC7N in the three outflow sources I20582, L1221 and
L1251A. Shocked carbon-chain chemistry (SCCC) is proposed to explain the
abnormal high abundances of C3S compared with those of nitrogen-bearing CCMs.
Gas-grain chemical models support the idea that shocks can fuel the environment
of those sources with enough thus driving the generation of S-bearing
CCMs.Comment: 7 figures, 8 tables, accepted by MNRA
A particular carbon-chain-producing region: L1489 starless core
We detected carbon-chain molecules (CCMs) HC2n+1N (n = 1−3) and C3S in Ku band as well as high-energy excitation lines including C4H N = 9–8, J = 17/2–15/2, 19/2–17/2, and CH3CCH J = 5–4, K = 2 in the 3 mm band toward a starless core called the eastern molecular core (EMC) of L1489 IRS. Maps of all the observed lines were also obtained. Comparisons with a number of early starless cores and the warm carbon-chain chemistry (WCCC) source L1527 show that the column densities of C4H and CH3CCH are close to those of L1527, and the CH3CCH column densities of the EMC and L1527 are slightly higher than those of TMC-1. The EMC and L1527 have similar C3S column densities, but they are much lower than those of all the starless cores, with only 6.5 and 10% of the TMC-1 value, respectively. The emissions of the N-bearing species of the EMC and L1527 are at the medium level of the starless cores. These comparisons show that the CCM emissions in the EMC are similar to those of L1527, though L1527 contains a protostar. Although dark and quiescent, the EMC is warmer and at a later evolutionary stage than classical carbon-chain–producing regions in the cold, dark, quiescent early phase. The PACS, SPIRE, and SCUBA maps evidently show that the L1489 IRS seems to be the heating source of the EMC. Although it is located at the margins of the EMC, its bolometric luminosity and bolometric temperature are relatively high. Above all, the EMC is a rather particular carbon-chain-producing region and is quite significant for CCM science