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低红移IGM的HST/COS调查。I.调查、方法和总体结果

An HST/COS Survey of the Low-Redshift IGM. I. Survey, Methodology, & Overall Results

Charles W. Danforth, Brian A. Keeney, Evan M. Tilton, J. Michael Shull, Matthew Stevans, Matthew M. Pieri, John T. Stocke, Blair D. Savage, Kevin France, David … 展开作者

Charles W. Danforth, Brian A. Keeney, Evan M. Tilton, J. Michael Shull, Matthew Stevans, Matthew M. Pieri, John T. Stocke, Blair D. Savage, Kevin France, David Syphers, Britton D. Smith, James C. Green, Cynthia Froning, Steven V. Penton, Steven N. Osterman

摘要:

我们使用高质量、中等分辨率的{ \it哈勃太空望远镜}/宇宙起源摄谱仪(\HST /COS)观测82个红移为$z_{AGN}<0.85$的紫外亮活动星系核,以构建迄今为止对低红移星系际介质(IGM)的最大调查:HI和25种不同金属中的5343条河外吸收线在$z_{abs}<0.75$中,离子种类被分为2610个不同的红移系统,覆盖了总的红移路径长度$Δz_{HI}=21.7$和$Δz_{OVI}=14.5$。我们的半自动寻线和测量技术使目录尽可能客观地定义。HI系统的累积柱密度分布可以用$dN(>N)/dz=C_{14}(N/10^{14} cm^{-2})^{-(β-1)}$、$C_{14}=25\pm1$和$β=1.65\pm0.02$参数化。对于$z<0.47$,可以看到该分布在幅度$C_{14}\sim(1+z)^{2.0\pm0.1}$和斜率$β(z)=1.73-0.26 z$上都发生演变。我们观察了427个系统中的金属线,发现在金属中检测到的IGM吸收体的分数强烈依赖于N_{HI}。OVI吸收剂的分布似乎与Lya森林的演变相同。我们计算的贡献$Ω_b$从不同的组成部分的低$z$ IGM和确定的Lya减量作为红移的函数。IGM吸波器通过两点相关函数(TPCF)在速度空间进行了分析。我们发现\HI \吸收剂在$Δv=50-300$ km/s的尺度上大量聚集,在$Δv>1000$ km/s没有显著的聚集。将样品分成强吸收体和弱吸收体,我们看到大多数聚簇发生在强的、含$N_{HI}>10^{13.5} cm^{-2}$金属的IGM系统中。吸收线和完全还原光谱的完整目录可通过MAST作为高级科学产品在http://archive.stsci.edu/prepds/igm/上获得。

英文摘要:

We use high-quality, medium-resolution {\it Hubble Space Telescope}/Cosmic Origins Spectrograph (\HST/COS) observations of 82 UV-bright AGN at redshifts $z_{AGN}<0.85$ to construct the largest survey of the low-redshift intergalactic medium (IGM) to date: 5343 individual extragalactic absorption lines in HI and 25 different metal-ion species grouped into 2610 distinct redshift systems at $z_{abs}<0.75$ covering total redshift pathlengths $Δz_{HI}=21.7$ and $Δz_{OVI}=14.5$. Our semi-automated line-finding and measurement technique renders the catalog as objectively-defined as possible. The cumulative column-density distribution of HI systems can be parametrized $dN(>N)/dz=C_{14}(N/10^{14} cm^{-2})^{-(β-1)}$, with $C_{14}=25\pm1$ and $β=1.65\pm0.02$. This distribution is seen to evolve both in amplitude, $C_{14}\sim(1+z)^{2.0\pm0.1}$, and slope $β(z)=1.73-0.26 z$ for $z<0.47$. We observe metal lines in 427 systems, and find that the fraction of IGM absorbers detected in metals is strongly dependent on N_{HI}. The distribution of OVI absorbers appear to evolve in the same sense as the Lya forest. We calculate contributions to $Ω_b$ from different components of the low-$z$ IGM and determine the Lya decrement as a function of redshift. IGM absorbers are analyzed via a two-point correlation function (TPCF) in velocity space. We find substantial clustering of \HI\ absorbers on scales of $Δv=50-300$ km/s with no significant clustering at $Δv>1000$ km/s. Splitting the sample into strong and weak absorbers, we see that most of the clustering occurs in strong, $N_{HI}>10^{13.5} cm^{-2}$, metal-bearing IGM systems. The full catalog of absorption lines and fully-reduced spectra is available via MAST as a high-level science product at http://archive.stsci.edu/prepds/igm/.

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