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首页> 外文期刊>The Astrophysical journal >INTERFEROMETRIC CO J = 2-1 EMISSION MAPPING OF THE PROTOPLANETARY NEBULA IRAS 19475+3119
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INTERFEROMETRIC CO J = 2-1 EMISSION MAPPING OF THE PROTOPLANETARY NEBULA IRAS 19475+3119

机译:干涉星云CO J = 2-1行星状星云IRAS的发射映射19475 + 3119

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摘要

We present ~2″ resolution interferometric maps of the ~(12)CO J = 2-1 emission in the PPN IRAS 19475+3119 obtained with OVRO. These data probe two distinct molecular components, namely, a slowly expanding shell and a fast bipolar outflow. We have used a spatiokinematic model of the ~(12)CO J = 2-1 emission to constrain the properties of these two components. The shell has inner and outer radii of R_(in) ~ 6.5 x 10~(16) cm and R_(out) ~ 2 x 10~(17) cm and expands at V_(exp) ~ 11 km s~(-1). The ~(12)CO J = 2-1 line wing emission arises in a bipolar structure that emerges from two diametrically opposite holes in the slow shell. The bipolar outflow is aligned with one of the two lobe pairs of the quadrupolar optical nebula (at P. A. ≈ 80?). Both the holes and the bipolar outflow are most likely the result of the interaction of fast, collimated post-AGB winds with the shell. The quadrupolar morphology of the optical nebula indicates two distinct bipolar post-AGB winds ejected in two different directions. The elongation of the optical counterpart of the shell (at P.A. ≈ —45°) and two similarly aligned CO clumps suggest that the slow shell has also been affected by the wind interaction. The expansion velocity in the bipolar outflow increases linearly with the distance from the nebula center and reaches V_(exp) = 30 km s~(-1) (projected) at the tips of the lobes. This velocity gradient yields a relatively long kinematical age of ~1900 yr, assuming an outflow inclination of i = 30° with respect to the plane of the sky; this age is comparable with the post-AGB lifetime estimated from the shell expansion velocity and inner radius. We derive a mean kinetic temperature of ~14 K and a total mass of ~0.4 solar mass. The collimation and linear momentum (P ~ 4 x 10~(38) g cm s~(-1)) of the outflow are unlikely to result from radiation pressure on dust grains.
机译:我们提出了用OVRO获得的PPN IRAS 19475 + 3119中〜(12)CO J = 2-1发射的〜2“分辨率干涉图。这些数据探究了两个截然不同的分子成分,即壳的缓慢膨胀和快速的双极流出。我们已使用〜(12)CO J = 2-1排放的时空动力学模型来约束这两个组件的特性。壳的内外半径分别为R_(in)〜6.5 x 10〜(16)cm和R_(out)〜2 x 10〜(17)cm,并在V_(exp)〜11 km s〜(-1)处扩展)。 〜(12)CO J = 2-1线状机翼发射出现在双极结构中,该结构从慢壳中的两个直径相对的孔中出来。双极流出与四极光学星云的两个波瓣对之一对准(在P. A.≈80°?)。孔和双极流出极有可能是快速,准直的AGB后风与壳层相互作用的结果。光学星云的四极形态表明在两个不同方向上喷出了两个截然不同的双极AGB后风。壳的光学对应部分的伸长(在P.A.≈-45°处)和两个类似排列的CO团块表明,慢壳也受到风相互作用的影响。双极流出的膨胀速度随着距星云中心距离的增加而线性增加,并在叶尖达到V_(exp)= 30 km s〜(-1)(投影)。假设相对于天空平面的流出倾角为i = 30°,则该速度梯度会产生相对较长的〜1900 yr的运动年龄。这个年龄与从壳膨胀速度和内半径估计的AGB后寿命相当。我们得出的平均动力学温度为〜14 K,总质量为〜0.4太阳质量。尘埃的辐射压力不太可能导致流出的准直和线性动量(P〜4 x 10〜(38)g cm s〜(-1))。

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