首页> 外文期刊>Astronomy and astrophysics >Molecular hydrogen in the zabs?=?2.66 damped Lyman-α absorber towards Q J?0643?5041 - Physical conditions and limits on the cosmological variation of the proton-to-electron mass ratio
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Molecular hydrogen in the zabs?=?2.66 damped Lyman-α absorber towards Q J?0643?5041 - Physical conditions and limits on the cosmological variation of the proton-to-electron mass ratio

机译:Zabs?=?2.66中的分子氢向Q J?0643?5041衰减了Lyman-α吸收剂-物理条件和质子电子质量比的宇宙学变化极限

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Context. Molecular hydrogen in the interstellar medium (ISM) of high-redshift galaxies can be detected directly from its UV absorption imprinted in the spectrum of background quasars. Associated absorption from H?i and metals allow for the study of the chemical enrichment of the gas, while the analysis of excited species and molecules make it possible to infer the physical state of the ISM gas. In addition, given the numerous H2 lines usually detected, these absorption systems are unique tools to constrain the cosmological variation of the proton-to-electron mass ratio, μ. Aims. We intend to study the chemical and physical state of the gas in the H2-bearing cloud at zabs???=???2.658601 towards the quasar Q J?0643?5041 (zem???=???3.09) and to derive a useful constraint on the variation of μ. Methods. We use high signal-to-noise ratio, high-resolution VLT-UVES data of Q J?0643?5041 amounting to a total of more than 23 h exposure time and fit the H?i, metals, and H2 absorption features with multiple-component Voigt profiles. We study the relative populations of H2 rotational levels and the fine-structure excitation of neutral carbon to determine the physical conditions in the H2-bearing cloud. Results. We find some evidence for part of the quasar broad-line emission region not being fully covered by the H2-bearing cloud. We measure a total neutral hydrogen column density of log??N(H?i)(cm-2)???=???21.03???±???0.08. Molecular hydrogen is detected in several rotational levels, possibly up to J?=?7, in a single component. The corresponding molecular fraction is log f = -2.19+0.07-0.08, where f?=?2N(H2)/(2N(H2)+?N(H?i)). The H2 Doppler parameter is of the order of 1.5 km?s-1 for J?=?0, 1, and 2 and larger for J> 2. The molecular component has a kinetic temperature of Tkin???80 K, which yields a mean thermal velocity of ~1 km?s-1, consistent with the Doppler broadening of the lines. The UV ambient flux is of the order of the mean ISM Galactic flux. We discuss the possible detection of HD and derive an upper limit of log??N(HD) ? 13.65?±?0.07 leading to log? HD/(2 × H2) ? ??5.19?±?0.07, which is consistently lower than the primordial D/H ratio. Metals span ~210 km?s-1 with [Zn/H] = ?0.91?±?0.09 relative to solar, with iron depleted relative to zinc [Zn/Fe] = 0.45?±?0.06, and with the rare detection of copper. We follow the procedures used in our previous works to derive a constraint on the cosmological variation of μ, Δμ/μ = (7.4?±?4.3stat?±?5.1syst)?×?10-6.
机译:上下文。高红移星系星际介质(ISM)中的分子氢可以直接从背景类星体光谱中所印记的紫外线吸收中检测出来。从H 2和金属的相关吸收可以研究气体的化学富集,而对受激物种和分子的分析则可以推断出ISM气体的物理状态。此外,考虑到通常会检测到大量H2线,这些吸收系统是限制质子与电子质量比μ的宇宙学变化的独特工具。目的我们打算研究朝向准星QJ?0643?5041(zem ??? = ??? 3.09)处zabs处含H2的云中气体的化学和物理状态。对μ变化的有用约束。方法。我们使用QJ?0643?5041的高信噪比,高分辨率VLT-UVES数据(总计超过23小时的暴露时间)来拟合H?i,金属和H2的吸收特性,并采用多个组件Voigt配置文件。我们研究了H2旋转水平的相对种群以及中性碳的精细结构激发,以确定含H2的云的物理条件。结果。我们发现一些证据表明类星体宽线发射区域的一部分未被含H2的云完全覆盖。我们测得的总中性氢柱密度为log 50 N(H 2)(cm-2)= 21.03±0.08。在单个成分中,分子氢以几个旋转水平被检测到,可能高达Jα=α7。相应的分子分数为log f = -2.19 + 0.07-0.08,其中f 1 =α2 N(H 2)/(2N(H 2)+αN(H -1))。对于J 1 =θ0,1和2,H 2多普勒参数约为1.5km 2 s-1,对于J> 2,H 2多普勒参数更大。该分子组分的动力学温度为Tkin≥80K,得到平均热速度约为1 km?s-1,与多普勒谱线展宽一致。 UV环境通量约为ISM Galactic平均通量。我们讨论了HD的可能检测,并推导出log ?? N(HD)?的上限。 13.65±0.07导致对数? HD /(2×H2)? 5.19±0.07,始终低于原始D / H比。金属跨度约为210 km?s-1,相对于太阳能,[Zn / H] =?0.91?±?0.09,相对于锌,铁耗竭[Zn / Fe] = 0.45?±?0.06,并且很少检测到铜。我们遵循先前工作中使用的程序,得出对μ宇宙学变化的约束,Δμ/μ=(7.4?±?4.3stat?±±5.1syst)?×?10-6。

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