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首页> 外文期刊>The Astrophysical journal >Tracing the Warm-Hot Intergalactic Medium at Low Redshift: X-Ray Forest Observations toward H1821+643
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Tracing the Warm-Hot Intergalactic Medium at Low Redshift: X-Ray Forest Observations toward H1821+643

机译:在低红移下追踪温暖的星系间介质:对H1821 + 643的X射线森林观测

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We present a high-resolution (λ/Δλ ≈ 500) X-ray spectrum of the bright quasar H1821+643 (z = 0.297), obtained in a 470 ks observation with the Chandra X-Ray Observatory. We search for X-ray absorption by highly ionized metal species, O VII and O VIII in particular, at the redshifts of the six intervening O VI absorption systems known from UV studies. We detect features with 2 σ significance at the predicted O VII and O VIII wavelengths of one O VI system, at the O VII wavelength of a second, and at the Ne IX wavelength of a third. We find two additional features of comparable strength (one O VII and one O VIII) within 1000 km s-1 of the O VI redshifts. The 1 σ constraints on the relative abundances of different species imply significant variations from system to system in f(O ), the fraction of oxygen in the O VI state. The constraints in the two detected O VI systems imply gas overdensities lower than the values δ 100 expected in virialized systems, suggesting that the absorption arises in lower density, filamentary structures. At the 2 σ level, however, the physical constraints are weak, although all of the systems must have temperature T 106 K to be consistent with upper limits on O VII. If we treat our 2 σ detections of known O VI systems as real, but assume minimal O VII and O VIII in the other systems, we estimate [f(O ) + f(O ) + f(O )]/f(O ) = 32 ± 9 for the average ratio of all highly ionized oxygen species to O VI. Combined with estimates of the total column density of O VI absorption per unit redshift, this ratio implies that the total baryon fraction associated with detected O VI absorbers is Ωb(O ) ~ 0.03 h, a substantial fraction of the baryon density predicted by big bang nucleosynthesis and larger than that associated with stars or with gas detected in 21 cm or X-ray emission. Because of the limited signal-to-noise ratio of the detections, these results must be treated with caution. Nonetheless, the combination of the O VI data with these X-ray forest measurements provides the most direct evidence to date for the pervasive, moderate-density, shock-heated intergalactic medium predicted by leading cosmological scenarios. The high inferred incidence of relatively strong O VII and O VIII absorption implies that some regions of the intergalactic medium are enriched to a level substantially above [O/H] = -1.
机译:我们展示了明亮的类星体H1821 + 643(z = 0.297)的高分辨率(λ/Δλ≈500)X射线光谱,该光谱是在钱德拉X射线天文台进行的470 ks观测中获得的。我们寻找高度离子化的金属物种,特别是O VII和O VIII的X射线吸收,这是从UV研究得知的六个介入的O VI吸收系统的红移。我们在一个O VI系统的预测O VII和O VIII波长,第二个O VII波长和第三个Ne IX波长处检测到具有2σ显着性的特征。我们在O VI红移的1000 km s-1内发现了两个强度相当的其他特征(一个O VII和一个O VIII)。不同物种的相对丰度的1σ约束意味着f(O)(O VI状态下的氧气份额)之间因系统而异。在两个检测到的O VI系统中的约束条件表明气体的密度低于在虚拟系统中预期的值δ100,这表明吸收发生在密度较低的丝状结构中。然而,在2σ级别,物理约束很弱,尽管所有系统必须具有T <106 K的温度才能与O VII的上限保持一致。如果我们将已知O VI系统的2σ次检测视为真实,但假设其他系统中的O VII和O VIII最小,则我们估计[f(O)+ f(O)+ f(O)] / f(O )= 32±9,表示所有高度电离的氧与O VI的平均比率。结合每单位红移的O VI吸收总柱密度估计值,该比率意味着与检测到的O VI吸收剂相关的总重子分数为Ωb(O)〜0.03 h,这是大爆炸所预测的重子密度的很大一部分核合成,并且比与恒星或21 cm或X射线发射中检测到的气体相关的合成更大。由于检测的信噪比有限,因此必须谨慎对待这些结果。尽管如此,O VI数据与这些X射线森林测量值的结合为迄今为止主要宇宙学情景所预测的普遍,中等密度,激波加热的星系间介质提供了最直接的证据。较高的O VII和O VIII吸收相对较高的推断发生率意味着银河中间介质的某些区域富集到实质上高于[O / H] = -1的水平。

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