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首页> 外文期刊>The Astrophysical journal >HIGHLY IONIZED GAS SURROUNDING HIGH-VELOCITY CLOUD COMPLEX C
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HIGHLY IONIZED GAS SURROUNDING HIGH-VELOCITY CLOUD COMPLEX C

机译:围绕高云度复合物C的高度电离的气体

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We present Far Ultraviolet Spectroscopic Explorer and Hubble Space Telescope observations of high-, intermediate-, and low-ion absorption in high-velocity cloud (HVC) Complex C along the lines of sight toward five active galaxies. Our purpose is to investigate the idea that Complex C is surrounded by an envelope of highly ionized material, arising from the interaction between the cloud and a hot surrounding medium. We measure column densities of high-velocity high-ion absorption and compare the kinematics of low-, intermediate-, and high-ionization gas along the five sight lines. We find that in all five cases, the H Ⅰ and O Ⅵ high-velocity components are centered within 20 km s~(-1) of one another, with an average displacement of = 3 +- 12 km s~(-1). In those directions where the H Ⅰ emission extends to more negative velocities (the so-called high-velocity ridge), so does the O Ⅵ absorption. The kinematics of Si Ⅱ is also similar to that of O Ⅵ, with < v_(O Ⅵ) - v_(Si Ⅱ)> = 0 +- 15 km s~(-1). We compare our high-ion column density ratios to the predictions of various models, adjusted to account for both recent updates to the solar elemental abundances and relative elemental abundance ratios in Complex C. Along the PG 1259+593 sight line, we measure N(Si Ⅳ)/N(O Ⅵ) = 0.10 +- 0.02, N(C Ⅳ)/N(O Ⅵ) = 0.351_(-0.06)~(+0.05), and N(N Ⅴ)/N(O Ⅵ) < 0.07 (3 σ). These ratios are inconsistent with collisional ionization equilibrium at one kinetic temperature. Photoionization by the extragalactic background is ruled out as the source of the high ions since the path lengths required would make HVCs unreasonably large; photoionization by radiation from the disk of the Galaxy also appears unlikely since the emerging photons are not energetic enough to produce O Ⅵ. By themselves, ionic ratios are insufficient to discriminate between various ionization models, but by considering the absorption kinematics as well, we consider the most likely origin for the highly ionized high-velocity gas to be at the conductive or turbulent interfaces between the neutral/warm ionized components of Complex C and a surrounding hot medium. The presence of interfaces on the surface of HVCs provides indirect evidence for the existence of a hot medium in which the HVCs are immersed. This medium could be a hot (T approx> 10~6 K) extended Galactic corona or hot gas in the Local Group.
机译:我们介绍了远紫外光谱资源管理器和哈勃太空望远镜对高速云(HVC)复杂C中沿五个活动星系的视线的高,中和低离子吸收的观测结果。我们的目的是研究由云和高温环境介质之间的相互作用引起的复合物C被高离子化材料包围的想法。我们测量高速高离子吸收的色谱柱密度,并比较沿五个视线的低,中和高电离气体的运动学。我们发现,在所有五种情况下,HⅠ和OⅥ高速分量都彼此位于20 km s〜(-1)的中心,平均位移 = 3 +-12 km s〜(-1)。在HⅠ发射扩展到更多负速度的那些方向(所谓的高速脊),OⅥ吸收也是如此。 SiⅡ的运动学也与OⅥ相似, = 0 +-15 km s〜(-1)。我们将高离子柱密度比与各种模型的预测值进行比较,并对其进行调整,以解决复合体C中太阳元素丰度和相对元素丰度比的最新更新。沿着PG 1259 + 593视线,我们测量N( SiⅣ)/ N(OⅥ)= 0.10 +-0.02,N(CⅣ)/ N(OⅥ)= 0.351 _(-0.06)〜(+0.05)和N(NⅤ)/ N(OⅥ) )<0.07(3σ)。这些比率与一个动力学温度下的碰撞电离平衡不一致。排除了河外背景的光电离作用,因为高离子源是必需的,因为所需的路径长度会使HVC变得过大。由于新兴的光子的能量不足以产生OⅥ,因此通过银河系盘的辐射进行电离也似乎不太可能。离子比率本身不足以区分各种电离模型,但是通过考虑吸收运动学,我们认为高电离高速气体最有可能的起源是中性/暖性之间的导电或湍流界面络合物C和周围热介质的电离组分。 HVC表面上的界面的存在提供了HVC浸入其中的热介质的间接证据。该介质可以是本地组中热(T约> 10〜6 K)扩展的银河电晕或热气。

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