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Echelle Spectroscopy of Interstellar Absorption toward μ Columbae with the Goddard High Resolution Spectrograph

机译:戈达德高分辨率光谱仪的星际对μColumbae吸收的Echelle光谱

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Goddard High Resolution Spectrograph echelle-mode observations of the interstellar absorption lines of Mg II, Si IV, C IV, and N V toward μ Columbae (HD 38666) are presented. The observations have a spectral resolution of 3.5 km s-1 and signal-to-noise ratios (S/Ns) of 20–200. The μ Col sight line (l = 2373, b = -271, d = 0.40 kpc, z = -0.18 kpc) extends though the Local Bubble and the warm neutral, warm ionized, and hot ionized phases of the interstellar medium (ISM). The high-ionization column densities toward μ Col are log N(Si IV) = 12.16 ± 0.05, log N(C IV) = 12.88 ± 0.02, and logN(N V) = 11.8–12.3. Profile fits to Copernicus satellite measures of O VI absorption toward μ Col yield log N(O VI) = 13.82±0.01 and b = 38.7 km s-1. This implies N(C IV)/N(O VI) = 0.11 ± 0.01, which is typical of the values found for the hot ISM of the Galactic disk. The O VI profile is twice as broad as the C IV and N V profiles, even though these species have roughly similar average velocities. Some of the C IV, N V, and O VI absorption toward μ Col may occur at the interface of the Local Cloud and Local Bubble, although additional contributions to these ions probably also occur in more distant gas along the sight line. A substantial part of the Si IV absorption likely arises in warm photoionized gas in an H II region surrounding μ Col. The profile width differences among the high-ionization lines of C IV, N V, and O VI could be produced if the line of sight passes through a highly evolved supernova remnant. The observations for μ Col and for other stars observed at high resolution with the GHRS reveal that multiple gas types (warm and hot) contribute to the absorption by the highly ionized atoms along both nearby and distant sight lines. Disentangling the relative contributions from the different gas types requires high-resolution and high-S/N observations. The Mg II observations, combined with a solar Mg reference abundance, imply that the Mg depletion toward μ Col is -0.31 dex. As observed for other sight lines through the warm neutral medium, the gas-phase observations of Mg, when combined with results for Fe and Si, suggest that Mg and Fe are more deficient from the gas phase than one would expect if these elements are only contained in silicate dust grains.
机译:戈达德高分辨率光谱仪对Mg II,Si IV,C IV和N V朝向μColumbae(HD 38666)的星际吸收线的阶梯观测。观测的光谱分辨率为3.5 km s-1,信噪比(S / Ns)为20-200。 μCol视线(l = 2373,b = -271,d = 0.40 kpc,z = -0.18 kpc)延伸穿过局部气泡以及星际介质(ISM)的热中性,电离和热电离阶段。朝向μCol的高电离柱密度为log N(Si IV)= 12.16±0.05,log N(C IV)= 12.88±0.02和logN(N V)= 11.8-12.3。轮廓符合哥白尼卫星测量的O VI吸收率,朝向μCol产量log N(O VI)= 13.82±0.01和b = 38.7 km s-1。这意味着N(C IV)/ N(O VI)= 0.11±0.01,这是银盘热ISM的典型值。 O VI剖面的宽度是C IV和N V剖面的两倍,即使这些物种的平均速度大致相似。对μCol的一些C IV,N V和O VI吸收可能发生在局部云和局部气泡的界面,尽管对这些离子的其他贡献也可能发生在沿视线更远的气体中。 Si IV吸收的很大一部分可能发生在μCol周围的H II区域中的热光电离气体中。如果视线较高,则C IV,NV和O VI的高电离谱线之间的轮廓宽度差异可能会产生穿过高度演化的超新星残余。用GHRS在高分辨率下对μCol和其他恒星的观测表明,多种气体类型(暖和热)有助于沿近视线和远视线的高电离原子的吸收。区分不同气体类型的相对贡献需要高分辨率和高信噪比的观测。 Mg II的观察结果与日照Mg参考丰度相结合,表明M对μCol的耗竭量为-0.31 dex。正如通过温暖的中性介质对其他视线所观察到的那样,将Mg的气相观察结果与Fe和Si的结果相结合,表明Mg和Fe在气相中的缺乏程度比人们仅将这些元素仅存在时所期望的低。包含在硅酸盐尘粒中。
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