2006
DOI: 10.1002/asna.200610672
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Theoretical aspects of relativistic spectral features

Abstract: The inner parts of black-hole accretion discs shine in X-rays which can be monitored and the observed spectra can be used to trace strong gravitational fields in the place of emission and along paths of light rays. This paper summarizes several aspects of how the spectral features are influenced by relativistic effects. We focus our attention onto variable and broad emission lines, origin of which can be attributed to the presence of orbiting patterns -spots and spiral waves in the disc. We point out that the … Show more

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Cited by 17 publications
(20 citation statements)
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“…The observed radiation flux is then obtained by integrating the intrinsic emission over the entire disc surface, from the inner edge (r = r in ) to the outer edge (r = r out ), weighted by the transfer function T (r e , φ e , θ o , a) determining the impact of relativistic energy change (Doppler and gravitational) as well as the lensing effect for a distant observer directed along the inclination angle θ o (see Cunningham 1975;Asaoka 1989;Karas et al 1992;Karas 2006).…”
Section: Black-hole Signatures In Accretion Disc Radiationmentioning
confidence: 99%
“…The observed radiation flux is then obtained by integrating the intrinsic emission over the entire disc surface, from the inner edge (r = r in ) to the outer edge (r = r out ), weighted by the transfer function T (r e , φ e , θ o , a) determining the impact of relativistic energy change (Doppler and gravitational) as well as the lensing effect for a distant observer directed along the inclination angle θ o (see Cunningham 1975;Asaoka 1989;Karas et al 1992;Karas 2006).…”
Section: Black-hole Signatures In Accretion Disc Radiationmentioning
confidence: 99%
“…In the inner regions of black hole accretion disks, emerging photons are strongly influenced by strong gravity (Kato et al 1998). The framework of General Relativity (GR) is needed to properly determine the resulting spectrum (Fabian et al 2000;Karas 2006;Matt 2006;Miller 2007). Relativistic effects include the energy shifts, both due to special relativity (Doppler effect) and GR (gravitational redshift), as well as the light bending aberration effects that are particularly prominent near the photon orbit: r ph = 3 GM/c 2 = 4.43 M/M ⊙ km for a non-rotating black hole (the radius of r ph decreases with the black hole spin increasing).…”
Section: Introductionmentioning
confidence: 99%
“…We define the redshift factor (e.g., Karas ) g=νobservedνlocal, with ν observed and ν local being the radiation frequency measured by the observer in infinity and in the close proximity of the accretion disc, respectively. Aiming to take the relativistic effects into account in the first approximation, we adopt the redshift factor (Pecháček et al ) g=R()R3R+sinφsinIR2+4()1+normalcos()φnormalsin()I1, where R stands for the radial coordinate, φ stands for the azimuthal coordinate, and I stands for the inclination parameter of the system.…”
Section: Reflection Spectral Line From Evolving Accretion Ringsmentioning
confidence: 99%