...
首页> 外文期刊>The Astrophysical journal >HH 110 JET NEAR-INFRARED IMAGING: THE OUTFLOW MIXING LAYER
【24h】

HH 110 JET NEAR-INFRARED IMAGING: THE OUTFLOW MIXING LAYER

机译:HH 110 JET近红外成像:流出混合层

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

We present near-infrared images of the Herbig-Haro 110 jet centered at the molecular hydrogen lines v = 1-0 (2.121 μm) and v = 2-1 (2.248 μm). In young stellar objects these lines are mostly excited by low-velocity shocks and the energy released by turbulent processes. The ratio of these lines provides us with a preliminary diagnostic of the molecular gas excitation. The HH 110 jet was selected for four reasons: (1) it has a complicated optical "turbulent" morphology, (2) it is close to a high-density circum-stellar environment (a molecular core), (3) it does not have an obvious driving source, and (4) theoretical models suggest that this object corresponds to the early stages of a jet-cloud collision. We find that the molecular hydrogen emission follows the optical Hα and [S II] emission in a "straight" section of the jet (the northern ~1′), but it becomes shifted westward and separated from the optical emission afterward. We suggest that these morphological properties of the molecular hydrogen emission are consistent with that of a boundary layer. The 2.248 μm emission is faint in most condensations, except for the B1, E1, H1, and P1 knots, where it is clearly detected. The ratio of the 2.121 μm to the 2.248 μm lines for these knots ranges from 4.5 to 7.5, which implies excitation temperatures of ~2400-3100 K. The brightest condensation, H, however, has a smaller ratio (~1.9) and a higher temperature (~5900 K), which suggests a nonisothermal jet structure. In those cases where the H_2 emission is likely to be due to shocks, the line ratios are small enough to be explained by either C- or J-type shocks.
机译:我们展示了以分子氢线v = 1-0(2.121μm)和v = 2-1(2.248μm)为中心的Herbig-Haro 110射流的近红外图像。在年轻的恒星物体中,这些线主要是由低速冲击和湍流释放的能量所激发。这些线的比率为我们提供了分子气体激发的初步诊断。选择HH 110射流的原因有四个:(1)它具有复杂的光学“湍流”形态,(2)它靠近高密度的恒星环境(分子核),(3)没有有明显的驱动源,并且(4)理论模型表明,该物体对应于急流云碰撞的早期阶段。我们发现,在射流的“笔直”部分(北部〜1'),分子氢的发射遵循光学Hα和[S II]的发射,但随后向西偏移并与光学发射分离。我们建议分子氢发射的这些形态学特性与边界层的形态学特性是一致的。除B1,E1,H1和P1结以外,在大多数凝结中,2.248μm的发射都比较微弱,可以很清楚地检测到。这些结的2.121μm线与2.248μm线的比率范围为4.5至7.5,这意味着激发温度为〜2400-3100K。然而,最亮的冷凝物H的比率较小(〜1.9),并且更高。温度(〜5900 K),表明是非等温射流结构。在那些可能由于冲击而产生H_2的情况下,线宽比足够小,可以用C型或J型冲击来解释。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号