首页> 外文期刊>The Astrophysical journal >A STUDY OF THE REIONIZATION HISTORY OF INTERGALACTIC HELIUM WITH FUSE AND THE VERY LARGE TELESCOPE
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A STUDY OF THE REIONIZATION HISTORY OF INTERGALACTIC HELIUM WITH FUSE AND THE VERY LARGE TELESCOPE

机译:星际氦与保险丝和超大望远镜的电离历史研究

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摘要

We obtained high-resolution Far Ultraviolet Spectroscopic Explorer (FUSE; R ~ 20,000) and Very Large Telescope (VLT; R ~ 45,000) spectra of the quasar HE 2347-4342 in order to study the properties of the intergalactic medium between redshifts z = 2.0 and 2.9. The high-quality optical spectrum allows us to identify approximately 850 H Ⅰ absorption lines with column densities between N~5x10~(11) and 10~(18) cm~(-2). The reprocessed FUSE spectrum extends the wavelength coverage of the He Ⅱ absorption down to an observed wavelength of 920 A. Source flux is detected to rest-frame wavelengths as short as ~237 A. Approximately 1400 He Ⅱ absorption lines are identified, including 917 He Ⅱ Lyα systems and some of their He Ⅱ Lyβ, Lyγ, and Lyδ counterparts. The ionization structure of He Ⅱ is complex, with approximately 90 absorption lines that are not detected in the hydrogen spectrum. These features may represent the effect of soft ionizing sources. The ratio η = N(He Ⅱ)/N(H Ⅰ) varies approximately from unity to more than a thousand, with a median value of 62 and a distribution consistent with the intrinsic spectral indexes of quasars. This provides evidence that the dominant ionizing field is from the accumulated quasar radiation, with contributions from other soft sources such as star-forming regions and obscured active galactic nuclei, which do not ionize helium. We find an evolution in η toward smaller values at lower redshift, with the gradual disappearance of soft components. At redshifts z > 2.7, the large but finite increase in the He Ⅱ opacity, τ = 5 +- 1, suggests that we are viewing the end stages of a reionization process that began at an earlier epoch. Fits of the absorption profiles of unblended lines indicate comparable velocities between hydrogen and He~+ ions. For line widths 6_(He~+) = ξb_H, we find ξ = 0.95 +- 0.12, indicating a velocity field in the intergalactic medium dominated by turbulence. At hydrogen column densities N < 3 x 10~(12) cm~(-2), the number of forest lines shows a significant deficit relative to a power law and becomes negligible below N = 10~(11) cm~(-2).
机译:我们获得了准星HE 2347-4342的高分辨率远紫外光谱浏览器(FUSE; R〜20,000)和超大望远镜(VLT; R〜45,000)的光谱,以研究红移z = 2.0之间的星系间介质的性质。和2.9。高质量的光谱使我们能够识别出大约850条HⅠ吸收线,其柱密度在N〜5x10〜(11)和10〜(18)cm〜(-2)之间。经过重新处理的FUSE光谱将HeⅡ吸收的波长范围扩展到观察到的920 A波长。检测到源通量到短帧波长(约237 A)。鉴定出大约1400 HeⅡ吸收线,包括917 He ⅡLyα系统及其一些HeⅡLyβ,Lyγ和Lyδ对应物。 HeⅡ的电离结构很复杂,在氢谱中没有检测到大约90条吸收线。这些特征可能代表了软电离源的作用。 η= N(HeⅡ)/ N(HⅠ)的比率大约从1到大于千不等,中位数为62,其分布与类星体的固有光谱指数一致。这提供了证据,表明主要的电离场来自累积的类星体辐射,来自其他软源(例如恒星形成区域和活动的银河核被遮挡)的贡献,这些元素不会使氦离子化。我们发现,随着软成分的逐渐消失,η在较低的红移下朝向较小的值演变。在红移z> 2.7时,HeⅡ不透明性大但有一定增加,τ= 5 +1,这表明我们正在观察在较早时期开始的电离过程的结束阶段。非混合线的吸收曲线的拟合表明氢和He〜+离子之间的速度相当。对于线宽6_(He〜+)=ξb_H,我们发现ξ= 0.95 +-0.12,表明在湍流为主的银河系介质中的速度场。在氢柱密度N <3 x 10〜(12)cm〜(-2)时,林线数相对于幂律显示出明显的不足,而在N = 10〜(11)cm〜(-2)以下可忽略不计。 )。

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