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Photoionization Models for High Density Gas

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arxiv 2011.10603 v2 pith:QL45GAH3 submitted 2020-11-20 astro-ph.HE

Photoionization Models for High Density Gas

classification astro-ph.HE
keywords highdensitiesatomiccalculationsintensitiesmodelsprocessesradiation
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Relativistically broadened and redshifted 6.4 -- 6.9 keV iron K lines are observed from many accretion powered objects, including X-ray binaries and active galactic nuclei (AGN). Existence of gas close to the central engine implies large radiation intensities and correspondingly large gas densities if the gas is to remain partially ionized. Simple estimates indicate that high gas densities are needed to allow survival of iron against ionization. These are high enough that rates for many atomic processes are affected by mechanisms related to interactions with nearby ions and electrons. Radiation intensities are high enough that stimulated processes can be important. Most models currently in use for interpreting relativistic lines use atomic rate coefficients designed for use at low densities and neglect stimulated processes. In our work so far we have presented atomic structure calculations with the goal of providing physically appropriate models at densities consistent with line-emitting gas near compact objects. In this paper we apply these rates to photoionization calculations, and produce ionization balance curves and X-ray emissivities and opacities which are appropriate for high densities and high radiation intensities. The final step in our program will be presented in a subsequent paper: Model atmosphere calculations which incorporate these rates into synthetic spectra.

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Cited by 1 Pith paper

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  1. Fe K$\alpha$ line from the Broad Line Region of PDS456 with XRISM/Resolve

    astro-ph.HE 2026-07 conditional novelty 7.0

    XRISM/Resolve reveals a narrow, blueshifted neutral Fe Kα line (EW ≈ 9 eV, v_out ≈ 2700 km/s) in quasar PDS 456, likely from the outer Broad Line Region at the high-luminosity end of the X-ray Baldwin effect.