2022MNRAS.512.2961M


Query : 2022MNRAS.512.2961M

2022MNRAS.512.2961M - Mon. Not. R. Astron. Soc., 512, 2961-2971 (2022/May-2)

X-ray simulations of polar gas in accreting supermassive black holes.

McKAIG J., RICCI C., PALTANI S. and SATYAPAL S.

Abstract (from CDS):

Recent observations have shown that a large portion of the mid-infrared (MIR) spectrum of active galactic nuclei (AGNs) stems from the polar regions. In this paper, we investigate the effects of this polar gas on the X-ray spectrum of AGNs using ray-tracing simulations. Two geometries for the polar gas are considered, (1) a hollow cone corresponding to the best-fitting MIR model and (2) a filled cone, both with varying column densities (ranging from 1021 to 1022.5 cm–2) along with a torus surrounding the central X-ray source. We find that the polar gas leads to an increase in the equivalent width of several fluorescence lines below ∼5 keV (e.g. O, Ne, Mg, Si). A filled geometry is unlikely for the polar component, as the X-ray spectra of many type 1 AGNs would show signatures of obscuration. We also consider extra emission from the narrow-line region such as a scattered power law with many photoionized lines from obscured AGNs, and different opening angles and matter compositions for the hollow cone. These simulations will provide a fundamental benchmark for current and future high spectral resolution X-ray instruments, such as those onboard XRISM and Athena.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): atomic processes - galaxies: active - galaxies: Seyfert - X-rays: galaxies - X-rays: general

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
2 NGC 3393 Sy2 10 48 23.4653152920 -25 09 43.487648784   13.10 13.95 11.67 12.2 ~ 471 1
3 NAME Circinus Galaxy Sy2 14 13 09.906 -65 20 20.47   10.89 9.84 10.6 10.0 ~ 1331 1

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