We present observations of the O VI system at z_abs = 0.495096 toward PKS 0405-123 (z_em = 0.5726) obtained with FUSE and STIS. In addition to strong O VI, with log N(O VI) = 14.47+/-0.02, and moderate H I this absorber shows C III, N IV, O IV, and O V, with upper limits for another seven ions. The large number of available ions allows us to test ionization models usually adopted with far less contraints. We find the ionic column densities cannot be matched by collisional ionization models, in or out of equilibrium. Photoionization models can match the observed column densities, including O VI. If one assumes photoionization by a UV background dominated by QSOs, the metallicity of the gas is [O/H] = -0.15, while a model for the UV background with contributions from ionizing photons escaping from galaxies gives [O/H] = -0.62. Both give [N/O] ~ -0.6 and [C/H] ~ -0.2 to -0.1. The choice of ionizing spectrum is poorly constrained. Multiphase models with a contribution from both photoionized gas (at T~10^4 K) and collisionally ionized gas (at T~(1-3)x10^5 K) can also match the observations giving very similar metallicities. The O VI in this system is not necessarily a reliable tracer of WHIM matter. We do not detect Ne VIII or Mg X absorption. The limit on Ne VIII/O VI < 0.21 (3 sigma), the lowest yet observed. Thus this absorber shows no firm evidence of the "warm-hot intergalactic medium" at T~(0.5-3)x10^6 K thought to contain a significant fraction of the baryons at low redshift. We present limits on the total column of warm-hot gas in this absorber as a function of temperature. This system would be unlikely to provide detectable X-ray absorption in the ions O VII or O VIII even if it resided in front of the brighter X-ray sources in the sky.
Do the environmental conditions affect the dust-induced fragmentation in low-metallicity clouds ?: Effect of pre-ionization and far-ultraviolet/cosmic-ray fields
Probing the metallicity and ionization state of the circumgalactic medium at z~6 and beyond with OI absorption
低电离金属吸收由于OI已被确定为一个重要的探针的物理状态的星际/环星系介质在尾端的再电离。我们在此使用高分辨率流体动力学模拟来解释由Becker等人(2011)观察到的z~6处OI吸收剂的发生率。我们推断弱OI吸收体(EW > 0.1A)在亚DLAs范围内具有典型的HI柱密度,密度为平均重子密度的80倍,金属丰度约为太阳的1/500。这与在z~3处类似密度下推断的金属丰度相似,表明低质量星系周围环星系介质的金属富集在z~6时已经有了相当大的进展。红移范围5<z 5内OI吸收发生率的明显快速演变<6 mirrors that of self-shielded Lyman-Limit systems at lower redshift and is mainly due to the rapid decrease of the meta-galactic photo-ionization rate at z>。我们预测,随着IGM变得更加中性,OI吸收体的发生率将随着红移的增加而继续迅速上升。如果金属的分布延伸到较低密度的区域,OI吸收剂将允许探测宇宙网络中越来越中性的附属结构的金属富集。
Elevated Hot Gas and High-Mass X-ray Binary Emission in Low Metallicity Galaxies: Implications for Nebular Ionization and Intergalactic Medium Heating in the Early Universe
Spatially resolved metallicity and ionization in the merging system Gz9p3 at z=9.3
Stockholm University(斯德哥尔摩大学);Centro de Astrobiología (CAB), CSIC-INTA(天体生物学中心(CAB),西班牙国家研究委员会-国家航空技术研究所);Space Telescope Science Institute (STScI)(太空望远镜科学研究所);University of Copenhagen(哥本哈根大学);UK Astronomy Technology Centre, Royal Observatory Edinburgh(英国天文学技术中心,爱丁堡皇家天文台)