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arXiv 0801.0674astro-ph
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多极Post-AGB星IRAS 16594-4656的动力学和H_2形态

Kinematics and H_2 morphology of the multipolar Post-AGB star IRAS 16594-4656

G. C. Van de Steene, T. Ueta, P. A. M. van Hoof, M. Reyniers, A. G. Ginsburg

摘要:

IRAS 16594-4656的光谱显示了冲击激发的H_2发射和碰撞激发的发射谱线,如[O I],[C I]和[Fe II]。目标:目标是确定H_2和[Fe II]激波发射的位置,确定激波速度,并约束激波中的物理性质。方法:用近红外光谱仪Phoenix获得了H_2 - 1-0 S(1),H_22 -1 S(1),[Fe II]和Pa $β$发射线的高分辨光谱。结果:给出了H_2 - 1-0 S(1)、H_22 -1 S(1)和[Fe Ⅱ]的位置-速度图。H_2和[Fe Ⅱ]发射在空间上是扩展的。碰撞激发的[O I]和[C I]光发射谱线具有与提取的H_2谱线相似的双峰谱线,似乎是在同一激波中产生的。它们都表明膨胀速度约为8 km/s,并且存在一个中性的、非常高密度的区域,其中$n_{\rm e}$约为3 x 10^6至5 x 10^7 cm $^{-3}$。而[Fe II]的发射是单峰的。它的高斯半高宽为30 km/s,在峰值的1%处的总宽度为62 km/s。Pa $β$廓线更宽,高斯半高宽为48 km/s,在峰值的1%处的总宽度为75 km/s。结论:H $_2$的发射是在一个缓慢的5至20公里/秒的冲击波中激发到密集的物质在边缘的叶片,造成的相互作用的AGB喷出物和后AGB风。H_2数据的三维表示显示了在赤道区H_2发射较少的中空结构。[Fe II]发射不存在于叶片中,但起源于靠近中心恒星的快速冲击后AGB风或磁盘中。Pa $β$的发射似乎也起源于恒星附近。

英文摘要:

context: The spectrum of IRAS 16594-4656 shows shock excited H_2 emission and collisionally excited emission lines such as[O I],[C I],and [Fe II]. aim: The goal is to determine the location of the H_2 and [Fe II] shock emission, to determine the shock velocities,and constrain the physical properties in the shock. methods: High resolution spectra of the H_2 1-0 S(1),H_2 2-1 S(1), [Fe II], and Pa$β$ emission lines were obtained with the near infrared spectrograph Phoenix on Gemini South. results: The position-velocity diagrams of H_2 1-0 S(1), H_2 2-1 S(1), and [Fe II] are presented. The H_2 and [Fe II] emission is spatially extended. The collisionally excited [O I] and [C I] optical emission lines have a similar double peaked profile compared to the extracted H_2 profile and appear to be produced in the same shock. They all indicate an expansion velocity of ~8 km/s and the presence of a neutral, very high density region with $n_{\rm e}$ about 3 x 10^6 to 5 x10^7 cm$^{-3}$. The [Fe II] emission however is single peaked. It has a gaussian FWHM of 30 km/s and a total width of 62 km/s at 1% of the peak. The Pa$β$ profile is even wider with a gaussian FWHM of 48 km/s and a total width of 75 km/s at 1% of the peak. conclusions: The H$_2$ emission is excited in a slow 5 to 20 km/s shock into dense material at the edge of the lobes, caused by the interaction of the AGB ejecta and the post-AGB wind. The 3D representation of the H_2 data shows a hollow structure with less H_2 emission in the equatorial region. The [Fe II] emission is not present in the lobes, but originates close to the central star in fast shocks in the post-AGB wind or in a disk. The Pa$β$ emission also appears to originate close to the star.

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