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A PARSEC-SCALE HERBIG-HARO JET IN BARNARD 5

机译:巴纳德5的PARSEC规模的HERBIG-HARO喷气式飞机

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We report the discovery of a parsec-scale, jetlike, bipolar Herbig-Haro flow, HH 366, emerging from the young stellar object IRS 1, which is embedded in the dark cloud Barnard 5 (B5) at the eastern end of the Perseus molecular cloud complex. The jet is about 22' in extent, which corresponds to a projected length of about 2.2 pc (assuming a distance of 350 pc), and is less than 1' (0.1 pc) wide. The brighter southwestern end of the jet is receding, with a velocity between 30 and 100 km s~(-1). The fainter eastern lobe is blueshifted with a slightly lower radial velocity amplitude. The blueshifted jet emerges from IRS 1 at a position angle of about 75°. Both the redshifted and blueshifted portions of the flow are brightest at their ends (the most distant points from the source). In the blueshifted eastern lobe, faint emission can be traced to within several arcminutes of the source, while the redshifted lobe emerges from behind the cloud core about 5' southwest of IRS 1. The orientation and kinematics of the Herbig-Haro jet matches that of the inner portion of the CO outflow from IRS 1 mapped at high-angular resolution by Fuller et al. A reanalysis of the Goldsmith et al. ~(12)CO data shows that an envelope of high-velocity molecular gas extends from IRS 1 to both the eastern and western ends of the Herbig-Haro jet. The redshifted lobe of CO emission lying several arc-minutes north of IRS 3 (an infrared source located about 10' to the southwest of IRS 1) coincides with the southwestern (redshifted) optical lobe of the B5 jet. Although previously associated with IRS 3, this lobe is the brightest portion of the southwestern lobe of the IRS 1 CO outflow. Both the CO flow and the HH jet are nearly orthogonal to a 0.06 pc long ridge or extended "pseudodisk" of dense molecular gas seen in tracers such as HCN. The two lobes of the IRS 1 optical outflow are misaligned; the red-shifted lobe appears to be deflected south with respect to the axis inferred by connecting B5 IRS 1 to the end of the blueshifted lobe. A roughly 5-10 km s~(-1) motion of the source with respect to the host cloud could produce this misalignment. The IRS 1 outflow provides evidence for outflow models in which CO is entrained from dense molecular gas by a hypersonic jet. A second Herbig-Haro flow, HH 367, is located 1' southeast (at position angle 155°) of the infrared source B5 IRS 3.
机译:我们报告发现了一个从幼小恒星物体IRS 1出现的,具有百秒尺度,喷射状,双极的Herbig-Haro流HH 366的发现,IRS 1嵌在英仙座分子东端的暗云Barnard 5(B5)中云复杂。射流的范围大约为22',对应于大约2.2 pc(假定距离为350 pc)的投影长度,并且小于1'(0.1 pc)宽。喷气机西南端更明亮,速度在30至100 km s〜(-1)之间。较弱的东部肺叶呈蓝移,径向速度幅度略低。蓝移的射流以大约75°的位置角从IRS 1发出。流的红移和蓝移部分在其末端(离源最远的点)最亮。在蓝移的东部波瓣中,微弱的发射可追溯到源的几弧分之内,而红移的波瓣从IRS 1西南5'处的云芯后面出现。Hertig-Haro射流的方向和运动学与Fuller等人以高角度分辨率绘制的IRS 1中CO流出的内部部分。对金史密斯等人的重新分析。 〜(12)CO数据显示,高速分子气体的包层从IRS 1延伸到Herbig-Haro射流的东端和西端。位于IRS 3以北数弧分钟(红外光源位于IRS 1西南约10')处的CO排放的红移波瓣与B5射流的西南(红移)光学波瓣重合。尽管先前与IRS 3相关,但该叶是IRS 1 CO流出西南西南叶中最亮的部分。 CO流量和HH射流都几乎垂直于0.06 pc长的脊或在诸如HCN等示踪剂中看到的稠密分子气体的扩展“伪盘”。 IRS 1光学流出的两个波瓣未对准。通过将B5 IRS 1连接到蓝移瓣的末端,红移瓣似乎相对于所推断的轴向南偏斜。源相对于宿主云大约5-10 km s〜(-1)的运动可能会导致这种失准。 IRS 1流出为流出模型提供了证据,在该模型中,高超声速射流从浓分子气体中夹带了CO。第二个Herbig-Haro流HH 367位于红外源B5 IRS 3的东南1'(位置角155°)。

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