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Observations of CO J = 3-2 in the Outflow of the Starburst Galaxy M82

机译:星暴M82流出时CO J = 3-2的观测值

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Observations are presented of the distribution of 12CO J = 3-2 emission in the starburst galaxy M82 covering a region 3'' × 3'' (2.8 × 2.8 kpc). This area includes the halo region involved in the superwind outflow. More limited coverage is presented for 13CO J = 3-2 and C18O J = 3-2. The mass of molecular gas in the halo is about 5 × 108 M☉, with a dynamical timescale of the order of 107 yr. The results show the region of the outflow at higher CO excitation than previous published observations. Comparison with recently made observations of 12CO J = 2-1 shows that the CO gas becomes progressively de-excited at larger distances from the starburst disk, and the isotopic ratio 13CO/12CO J = 3-2 also becomes smaller outside the starburst disk. These effects are interpreted as differences in excitation and optical depth between the starburst region and the outflow and outer disk. A comparison between the 12CO J = 3-2 emission with a published 850 μm continuum map shows that CO makes a significant contribution to the continuum in this band and that the fractional contribution is greatest near ±30'' from the nucleus approximately along the major axis. The progressively slower rotation of the halo gas with distance above and below the disk, coupled with consideration of the conservation of angular momentum, is analyzed to reveal the pattern of the outflow. The flow appears to diverge more strongly below the disk, with a cone angle of about 90°, which compares to about 40° above the disk. The mass and energetics of the halo molecular gas suggest the possibility that the molecular material and dust in the halo will not escape from M82 but are instead being recycled through the halo after injection as supershells by one or more transient starburst events.
机译:观察到了在覆盖3''×3''(2.8×2.8 kpc)区域的星爆星系M82中12CO J = 3-2发射的分布。该区域包括超风流出所涉及的晕圈区域。对于13CO J = 3-2和C18O J = 3-2,提出了更有限的覆盖范围。晕圈中的分子气体质量约为5×108M☉,动态时标约为107年。结果显示,与以前发表的观察结果相比,在更高的CO激发下流出的区域。与最近所作的12CO J = 2-1的观察结果的比较表明,CO气体在距星爆盘较大的距离处逐渐消散,并且同位素比13CO / 12CO J = 3-2在星爆盘外也变小。这些效应被解释为星爆区域与流出和外盘之间在激发和光学深度方面的差异。将12CO J = 3-2发射与已发布的850μm连续谱图进行比较,结果表明CO在该谱带中对连续谱有重要贡献,并且在主要原子核附近±30''处,分数贡献最大。轴。分析了随着距离圆盘上方和下方的距离逐渐变慢的卤代气体旋转,并考虑了角动量守恒,揭示了流出的模式。流量似乎在圆盘下方发散得更强烈,锥角约为90°,而圆盘上方的锥角约为40°。晕圈分子气体的质量和能量表明,晕圈中的分子材料和尘埃不会从M82逸出,而是在注入后作为一个超级壳通过一个或多个瞬态星爆事件通过晕圈再循环。

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