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首页> 外文期刊>The Astrophysical journal >Far Ultraviolet Spectroscopic Explorer Observations of Molecular Hydrogen in Translucent Interstellar Clouds. II. The Line of Sight toward HD 110432
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Far Ultraviolet Spectroscopic Explorer Observations of Molecular Hydrogen in Translucent Interstellar Clouds. II. The Line of Sight toward HD 110432

机译:半透明星际云中分子氢的远紫外光谱浏览器观察。二。朝向HD 110432的视线

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We report the second study from the FUSE survey of molecular hydrogen in translucent clouds for the line of sight toward HD 110432. This star lies beyond the Coalsack dark nebula, and, with E(B-V) = 0.40 and AV = 1.32, this line of sight bridges the gap between less-extinguished diffuse-cloud lines of sight with AV ~ 1, such as ζ Ophiuchi, and translucent-cloud lines of sight with AV 2, such as HD 73882. Through profile fitting and a curve-of-growth analysis, we have derived rotational populations for H2 for J = 0-7. The line of sight has a total molecular hydrogen column density, log N(H2) = 20.68 ± 0.05 cm-2, nearly identical to that toward ζ Oph but a factor of 3 less than that toward HD 73882. The ratio of N(J = 1) to N(J = 0) yields a kinetic temperature Tkin = 63 ± 7 K, which is similar to other lines of sight with AV 1. The high-J lines show considerable excitation above this temperature. However, the high-J lines cannot be well fitted to a single excitation temperature, and the even-J lines of para-hydrogen appear slightly enhanced relative to the odd-J lines of ortho-hydrogen. The high-J excitation is similar to that toward ζ Oph but is much smaller than that toward HD 73882. Chemical modeling indicates that the physical conditions in the cloud(s) are very similar to those in the cloud(s) toward ζ Oph. An analysis of IUE spectra of the Lyα line gives N(H I) = 20.85 ± 0.15 cm-2. Combined with N(H2), we derive a hydrogen molecular fraction, f = 0.58 ± 0.12, statistically identical to that found for the lines of sight toward ζ Oph and HD 73882. From the FUSE data and a curve-of-growth analysis using the same component structure as H2, we find log N(HD) = 15.2 cm-2, which is between the values found for ζ Oph and HD 73882. Profile fitting suggests smaller b values for HD than for H2, and log N(HD) = 16.0 cm-2. From FUSE and IUE data, we derive log N(CO) ≈ 14.3 cm-2, assuming the same component structure as CH or log N(CO) ≈ 14.8 cm-2, if all observed CO is cospatial with the strongest CH component. From the combined measurements of hydrogen- and carbon-containing molecules, the line of sight toward HD 110432 appears quite similar to the diffuse-cloud line of sight toward ζ Oph and quite dissimilar to the translucent-cloud line of sight toward HD 73882. Upcoming FUSE observations will further explore the transition between diffuse and translucent clouds.
机译:我们报告了FUSE调查的半透明云中分子氢朝向HD 110432的视线的第二项研究。该恒星位于Coalsack暗星云之外,并且在E(BV)= 0.40和AV = 1.32的情况下,视线弥合了AV〜1时熄灭程度较低的弥散云视线(例如ζ蛇夫座)和AV 2时的半透明云视线(例如HD 73882)之间的间隙。通过轮廓拟合和曲线增长分析,我们得出了J = 0-7的H2的旋转种群。视线的总氢分子列密度为log N(H2)= 20.68±0.05 cm-2,与朝向ζOph时几乎相同,但比朝向HD 73882时小3倍。N(J = 1)到N(J = 0)会产生动力学温度Tkin = 63±7 K,这与AV 1的其他视线相似。高J线在此温度以上显示出相当大的激发。但是,高J谱线不能很好地适应单个激发温度,并且相对于原氢的奇J谱线,对氢的偶数J谱线似乎略有增强。高J激发类似于朝向ζOph的激发,但远小于朝向HD 73882的激发。化学建模表明,云中的物理条件与针对ζOph的云中的物理条件非常相似。对Lyα线的IUE谱进行分析,得出N(H I)= 20.85±0.15 cm-2。结合N(H2),我们得出氢分子分数f = 0.58±0.12,在统计学上与朝向ζOph和HD 73882的视线所见的氢分子分数相同。从FUSE数据和使用与H2相同的组件结构,我们发现log N(HD)= 15.2 cm-2,介于ζOph和HD 73882的值之间。轮廓拟合显示HD的b值比H2小,log N(HD )= 16.0 cm-2。从FUSE和IUE数据,假设所有观察到的CO与最强的CH组分共空间,则假设与CH的组分结构相同,则推导出log N(CO)≈14.3 cm-2。从含氢和碳的分子的组合测量中,朝向HD 110432的视线看起来与朝向ζOph的弥散云视线非常相似,而与朝向HD 73882的半透明云视线非常不相似。 FUSE观测将进一步探索弥散云和半透明云之间的过渡。

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