The abundance and physical properties of O VII and O VIII X-ray absorption systems in the EAGLE simulations
arXiv:1904.01057 · doi:10.1093/mnras/stz1762
Abstract
We use the EAGLE cosmological, hydrodynamical simulations to predict the column density and equivalent width distributions of intergalactic O VII ( eV) and O VIII ( eV) absorbers at low redshift. These two ions are predicted to account for 40% of the gas-phase oxygen, which implies that they are key tracers of cosmic metals. We find that their column density distributions evolve little at observable column densities from redshift 1 to 0, and that they are sensitive to AGN feedback, which strongly reduces the number of strong (column density absorbers. The distributions have a break at , corresponding to overdensities of , likely caused by the transition from sheet/filament to halo gas. Absorption systems with are dominated by collisionally ionized O VII and O VIII, while the ionization state of oxygen at lower column densities is also influenced by photoionization. At these high column densities, O VII and O VIII arising in the same structures probe systematically different gas temperatures, meaning their line ratio does not translate into a simple estimate of temperature. While O VII and O VIII column densities and covering fractions correlate poorly with the H I column density at , O VII and O VIII column densities are higher in this regime than at the more common, lower H I column densities. The column densities of O VI and especially Ne VIII, which have strong absorption lines in the UV, are good predictors of the strengths of O VII and O VIII absorption and can hence aid in the detection of the X-ray lines.
Accepted for publication in MNRAS. Minor changes w.r.t version 1 including updated values for Table 2
References in corpus (9)
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- Clumpiness of Observed and Simulated Cold Circumgalactic Gas
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