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首页> 外文期刊>The Astrophysical journal >A Shock-induced Photodissociation Region in the HH 80/81 Flow: Far-Infrared Spectroscopy*
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A Shock-induced Photodissociation Region in the HH 80/81 Flow: Far-Infrared Spectroscopy*

机译:HH 80/81流中的冲击诱导的光解离区域:远红外光谱*

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摘要

The two spectrometers on board the Infrared Space Observatory were used to observe the Herbig-Haro objects HH 80, 81, and 80N, as well as their candidate exciting source IRAS 18162-2048. The fine structure lines of [O I] 63 μm, [O I] 145 μm, and [C II] 158 μm are detected everywhere, while [N II] 122 μm and [O III] 88.3 μm are only detected toward the HH objects; line ratios confirm for the first time the collisionally excited HH nature of HH 80N. No molecular line is detected in any of the observed positions. We use a full shock code to diagnose shock velocities vs ~ 100 km s-1 toward the HH objects, as expected from the optical spectroscopy. Since proper motions suggest velocities in excess of 600 km s-1, the HH objects probably represent the interface between two flow components with velocity differing by ~vs. Aside from the flow exciting source, the [C II] 158 μm line is everywhere brighter than the [O I] 63 μm line, indicating the presence of a photodissociation region (PDR) all along the flow. Continuum emission from the HH objects and from other positions along the flow is only detected longward of ~50 μm, and its proportionality to the [C II] 158 μm line flux suggests it is PDR in origin. We propose that the far-ultraviolet continuum irradiated by the HH objects and the jet is responsible for the generation of a PDR at the walls of the flow cavity. We develop a very simple model which strengthens the plausibility of this hypothesis.
机译:红外空间天文台上的两个光谱仪用于观察Herbig-Haro物体HH 80、81和80N,以及它们的候选激发源IRAS 18162-2048。到处都检测到[O I] 63μm,[O I] 145μm和[C II] 158μm的精细结构线,而[N II] 122μm和[O III] 88.3μm仅在朝向HH对象的位置检测到;线宽比首次确认了HN 80N的碰撞激发HH性质。在任何观察到的位置均未检测到分子线。正如光谱学所期望的,我们使用完整的冲击代码来诊断相对于HH对象的〜100 km s-1的冲击速度。由于适当的运动表明速度超过600 km s-1,因此HH对象可能代表两个流速差为〜vs的流动分量之间的界面。除了流动激发源之外,[C II] 158μm线到处都比[O I] 63μm线亮,表明整个流动过程中都存在光解离区(PDR)。从HH对象和沿流的其他位置的连续发射仅在〜50μm的较长位置被检测到,并且它与[C II] 158μm线通量成正比,表明其起源是PDR。我们建议由HH对象和射流照射的远紫外线连续体负责在流腔壁处产生PDR。我们开发了一个非常简单的模型,可以加强该假设的合理性。

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