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首页> 外文期刊>The Astrophysical journal >Chandra Discovery of a Tree in the X-Ray Forest toward PKS 2155–304: The Local Filament?
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Chandra Discovery of a Tree in the X-Ray Forest toward PKS 2155–304: The Local Filament?

机译:钱德拉(Chandra)在X射线森林中发现一棵朝向PKS 2155–304的树:本地细丝?

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摘要

We present the first X-ray detection of resonant absorption from warm/hot local gas either in our Galaxy, or in the intergalactic space surrounding our Galaxy, along the line of sight toward the blazar PKS 2155-304. The Chandra HRCS/LETG spectrum of this z = 0.116 source clearly shows, at ≥5 σ level, unresolved (FWHM ≤ 800 km s-1 at a 2 σ confidence level) O VII Kα and Ne IX Kα resonant absorption lines at 21.603 and 13.448 ? (i.e., cz = 14 km s-1 in the rest frame, from the O VII Kα line). O VIII Kα and O VII Kβ from the same system are also detected at a lower significance level (i.e., ~3 σ), while upper limits are set on O VIII Kβ, Ne X Kα, and Ne IX Kβ. The Far Ultraviolet Spectroscopic Explorer spectrum of this source shows complex O VI 2s→2p absorption at the same redshift as the X-ray system, made by at least two components: one relatively narrow (FWHM = 106 ± 9 km s-1) and slightly redshifted (cz = 36 ± 6 km s-1), and one broader (FWHM = 158 ± 26 km s-1) and blueshifted (cz = -135 ± 14 km s-1). We demonstrate that the physical states of the UV and X-ray absorbers are hard to reconcile with a single, purely collisionally ionized, equilibrium plasma. We propose instead that the X-ray and at least the broader and blueshifted UV absorber are produced in a low-density intergalactic plasma, collapsing toward our Galaxy, consistent with the predictions of a warm-hot intergalactic medium from numerical simulations. We find that any reasonable solution requires overabundance of Ne compared to O by a factor of ~2, with respect to the solar value. We propose several scenarios to account for this observation.
机译:我们向着blazar PKS 2155-304的视线提出了第一个X射线检测技术,该检测技术是在银河系或银河系周围的银河系空间中,从热/热的局部气体共振吸收的。 z = 0.116的源的Chandra HRCS / LETG谱清楚地表明,在≥5σ的水平下,未分辨的(在2σ置信度下的FWHM≤800 km s-1)O VIIKα和Ne IXKα在21.603和13.448? (即,从O VIIKα线到其余帧的cz = 14 km s-1)。来自同一个系统的O VIIIKα和O VIIKβ也以较低的显着性水平(即〜3σ)被检测到,而O VIIIKβ,Ne XKα和Ne IXKβ设置了上限。该源的远紫外光谱资源管理器光谱显示,在与X射线系统相同的红移下,复杂的O VI 2s→2p吸收由至少两个成分组成:一个相对较窄(FWHM = 106±9 km s-1)和略微红移(cz = 36±6 km s-1),再宽一点(FWHM = 158±26 km s-1),然后蓝移(cz = -135±14 km s-1)。我们证明了紫外线和X射线吸收剂的物理状态很难与单个纯碰撞离子化的平衡等离子体协调。相反,我们建议在低密度星际等离子体中产生X射线以及至少更宽泛的蓝移UV吸收剂,该等离子体向我们的银河塌陷,这与数值模拟对温暖热的星际介质的预测一致。我们发现,相对于太阳值,任何合理的解决方案都需要将Ne与O相比以2的倍数过量丰余。我们提出了几种方案来解释这种观察。

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