Effects of the refractive index of the X-ray corona on the emission lines in AGNs

X-ray reflection from an accretion disc produces characteristic emission lines allowing us to probe the innermost regions in active galactic nuclei. We investigate these emission lines under a framework of Riemannian geometrical optics where the corona has a refractive index of n ≠ 1. The empty spa...

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Bibliographic Details
Main Authors: Chainakun, P. (Author), Watcharangkool, A. (Author), Young, A.J (Author)
Format: Article
Language:English
Published: Oxford University Press 2022
Subjects:
Online Access:View Fulltext in Publisher
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020 |a 00358711 (ISSN) 
245 1 0 |a Effects of the refractive index of the X-ray corona on the emission lines in AGNs 
260 0 |b Oxford University Press  |c 2022 
300 |a 11 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1093/mnras/stac362 
520 3 |a X-ray reflection from an accretion disc produces characteristic emission lines allowing us to probe the innermost regions in active galactic nuclei. We investigate these emission lines under a framework of Riemannian geometrical optics where the corona has a refractive index of n ≠ 1. The empty space outside is a vacuum with n = 1. The Kerr metric is modified to trace the light rays that are bent due to not only the gravity of the black hole but also the effects of coronal plasma dependent on n. The choice of n alters the null geodesics, producing the effect which is analogous to the light deflection. For the corona with n > 1, the disc on the far side within the corona covers a larger area on the observer's sky, enhancing the blue wing of the line and producing more flux difference between the blue peak and extended red tail. The inverse effects are seen when n < 1. Moreover, the corona with n > 1 and n < 1 could induce extra shifts in the blue wing (Δgmax) to higher and lower energy, respectively. These effects are more prominent when the inclination angle is 60° and the corona extends to 5rg. To obtain the deviation of the line shift of Δgmax 0.01, the difference between the refractive index of the corona and that of the empty space must be Δ n ≳ 0.5 per cent. Finally, the lensing corona can influence the arrival time of photons that may affect the observed variability of these emission lines. © 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society. 
650 0 4 |a Accretion discs 
650 0 4 |a accretion, accretion discs 
650 0 4 |a Accretion: accretion disks 
650 0 4 |a black hole physics 
650 0 4 |a Black Hole physics 
650 0 4 |a Black holes 
650 0 4 |a Blue wings 
650 0 4 |a Characteristic emission 
650 0 4 |a Electromagnetic wave emission 
650 0 4 |a Emission lines 
650 0 4 |a Empty space 
650 0 4 |a Galaxies 
650 0 4 |a Galaxies active 
650 0 4 |a galaxies: active 
650 0 4 |a Geometrical optics 
650 0 4 |a Gravitation 
650 0 4 |a Light 
650 0 4 |a Refractive index 
650 0 4 |a Stars 
650 0 4 |a X-ray reflections 
650 0 4 |a X-rays: galaxies 
650 0 4 |a X-rays: Galaxies 
700 1 |a Chainakun, P.  |e author 
700 1 |a Watcharangkool, A.  |e author 
700 1 |a Young, A.J.  |e author 
773 |t Monthly Notices of the Royal Astronomical Society