TY - JOUR
T1 - Warm and dense molecular gas in the N 159 region:12CO J =4-3 and13CO J = 3-2 observations with NANTEN2 and ASTE
AU - Mizuno, Yoji
AU - Kawamura, Akiko
AU - Onishi, Toshikazu
AU - Minamidani, Tetsuhiro
AU - Muller, Erik
AU - Yamamoto, Hiroaki
AU - Hayakawa, Takahiro
AU - Mizuno, Norikazu
AU - Mizuno, Akira
AU - Stutzki, Jürgen
AU - Pineda, Jorge L.
AU - Klein, Uli
AU - Bertoldi, Frank
AU - Koo, Bon Chul
AU - Rubio, Monica
AU - Burton, Michael
AU - Benz, Arnold
AU - Ezawa, Hajime
AU - Yamaguchi, Nobuyuki
AU - Kohno, Kotaro
AU - Hasegawa, Tetsuo
AU - Tatematsu, Ke N.Ichi
AU - Ikeda, Masafumi
AU - Ott, Jürgen
AU - Wong, Tony
AU - Hughes, Annie
AU - Meixner, Margaret
AU - Indebetouw, Remy
AU - Gordon, Karl D.
AU - Whitney, Barbara
AU - Bernard, Jean Philippe
AU - Fukui, Yasuo
PY - 2010
Y1 - 2010
N2 - New 12CO J = 4-3 and 13CO J = 3-2 observations of the N159 region, an active site of massive star formation in the Large Magellanic Cloud, have been made with the NANTEN2 and ASTE submillimeter telescopes, respectively. The 12CO J = 4-3 distribution is separated into three clumps, each associated with N 159 W, N 159 E, and N 159 S. These new measurements toward the three clumps are used in coupled calculations of molecular rotational excitation and line radiation transfer, along with other transitions of the 12CO J = 1-0, J = 2-1, J = 3-2, and J = 7-6 as well as the isotope transitions of 13CO J = 1-0, J = 2-1, / = 3-2, and J = 4-3. The 13CO J = 3-2 data were newly taken for the present work. The temperatures and densities were found to be ∼ 70-80 K and ∼3 × 103cm-3 in N159 W and N159 E, and ∼30 K and ∼ 1.6 × 103cm-3 in N 159 S. These results were compared with the star-formation activity based on data of young stellar clusters and H II regions as well as midinfrared emission obtained with the Spitzer MIPS. The N159 E clump is associated with cluster(s) embedded, as observed at 24 μm by the Spitzer MIPS, and the derived high temperature, 80 K, is interpreted as being heated by these sources. The N159 E clump is likely to be responsible for a dark lane in a large H II region by dust extinction. On the other hand, the N 159 W clump is associated with clusters embedded mainly toward the eastern edge of the clump only. These clusters show offsets of 20"-40" from the 12CO J = 4-3 peak, and are probably responsible for heating indicated by the derived high temperature, 70 K. The N 159 W clump exhibits no sign of star formation toward the 12CO J = 4-3 peak position and its western region that shows enhanced R4-3/1-0 and R3-2/1-0 ratios. We therefore suggest that the N159 W peak represents a pre-star-cluster core of ∼ 105 M⊙ which deserves further detailed studies. The N159 S clump shows little sign of star formation, as is consistent with the lower temperature, 30 K, and has a somewhat lower density than N159 W and N 159 E. The N159 S clump is also a candidate for future star formation.
AB - New 12CO J = 4-3 and 13CO J = 3-2 observations of the N159 region, an active site of massive star formation in the Large Magellanic Cloud, have been made with the NANTEN2 and ASTE submillimeter telescopes, respectively. The 12CO J = 4-3 distribution is separated into three clumps, each associated with N 159 W, N 159 E, and N 159 S. These new measurements toward the three clumps are used in coupled calculations of molecular rotational excitation and line radiation transfer, along with other transitions of the 12CO J = 1-0, J = 2-1, J = 3-2, and J = 7-6 as well as the isotope transitions of 13CO J = 1-0, J = 2-1, / = 3-2, and J = 4-3. The 13CO J = 3-2 data were newly taken for the present work. The temperatures and densities were found to be ∼ 70-80 K and ∼3 × 103cm-3 in N159 W and N159 E, and ∼30 K and ∼ 1.6 × 103cm-3 in N 159 S. These results were compared with the star-formation activity based on data of young stellar clusters and H II regions as well as midinfrared emission obtained with the Spitzer MIPS. The N159 E clump is associated with cluster(s) embedded, as observed at 24 μm by the Spitzer MIPS, and the derived high temperature, 80 K, is interpreted as being heated by these sources. The N159 E clump is likely to be responsible for a dark lane in a large H II region by dust extinction. On the other hand, the N 159 W clump is associated with clusters embedded mainly toward the eastern edge of the clump only. These clusters show offsets of 20"-40" from the 12CO J = 4-3 peak, and are probably responsible for heating indicated by the derived high temperature, 70 K. The N 159 W clump exhibits no sign of star formation toward the 12CO J = 4-3 peak position and its western region that shows enhanced R4-3/1-0 and R3-2/1-0 ratios. We therefore suggest that the N159 W peak represents a pre-star-cluster core of ∼ 105 M⊙ which deserves further detailed studies. The N159 S clump shows little sign of star formation, as is consistent with the lower temperature, 30 K, and has a somewhat lower density than N159 W and N 159 E. The N159 S clump is also a candidate for future star formation.
KW - Galaxies: Magellanic clouds
KW - ISM: Clouds
KW - ISm: Molecules
KW - Stars: Formation
KW - Submillimeter
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U2 - 10.1093/pasj/62.1.51
DO - 10.1093/pasj/62.1.51
M3 - Article
AN - SCOPUS:77950572359
SN - 0004-6264
VL - 62
SP - 51
EP - 67
JO - Publications of the Astronomical Society of Japan
JF - Publications of the Astronomical Society of Japan
IS - 1
ER -