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General relativistic modelling of the negative reverberation X-ray time delays in AGN

General relativistic modelling of the negative reverberation X-ray time delays in AGN
General relativistic modelling of the negative reverberation X-ray time delays in AGN
We present the first systematic physical modelling of the time-lag spectra between the soft (0.3–1 keV) and the hard (1.5–4 keV) X-ray energy bands, as a function of Fourier frequency, in a sample of 12 active galactic nuclei which have been observed by XMMNewton. We concentrate particularly on the negative X-ray time-lags (typically seen above 10-4 Hz), i.e. soft-band variations lag the hard-band variations, and we assume that they are produced by reprocessing and reflection by the accretion disc within a lamp-post X-ray source geometry. We also assume that the response of the accretion disc, in the soft X-ray bands, is adequately described by the response in the neutral Fe Kα line at 6.4 keV for which we use fully general relativistic ray-tracing simulations to determine its time evolution. These response functions, and thus the corresponding time-lag spectra, yield much more realistic results than the commonly used, but erroneous, top-hat models. Additionally, we parametrize the positive part of the time-lag spectra (typically seen below 10-4 Hz) by a power law. We find that the best-fitting black hole (BH) masses, M, agree quite well with those derived by other methods, thus providing us with a new tool for BH mass determination. We find no evidence for any correlation between M and the BH spin parameter, α, the viewing angle, θ, or the height of the X-ray source above the disc, h. Also on average, the X-ray source lies only around 3.7 gravitational radii above the accretion disc and θ is distributed uniformly between 20° and 60°. Finally, there is a tentative indication that the distribution of α may be bimodal above and below 0.62.
accretion, accretion discs, black hole physics, relativistic processes, galaxies: active, galaxies: nuclei, x-rays: galaxies
1365-2966
3931-3950
Emmanoulopoulos, D.
ee2db4c6-3379-4604-8711-f779fb74f538
Papadakis, I.E.
81a6785c-8f4d-49a3-9eac-23ee4c743563
Dovciak, M.
574652ec-c6ab-4dfd-a44d-961f2c672791
Mchardy, I.
4f215137-9cc4-4a08-982e-772a0b24c17e
Emmanoulopoulos, D.
ee2db4c6-3379-4604-8711-f779fb74f538
Papadakis, I.E.
81a6785c-8f4d-49a3-9eac-23ee4c743563
Dovciak, M.
574652ec-c6ab-4dfd-a44d-961f2c672791
Mchardy, I.
4f215137-9cc4-4a08-982e-772a0b24c17e

Emmanoulopoulos, D., Papadakis, I.E., Dovciak, M. and Mchardy, I. (2014) General relativistic modelling of the negative reverberation X-ray time delays in AGN. Monthly Notices of the Royal Astronomical Society, 439 (4), 3931-3950. (doi:10.1093/mnras/stu249).

Record type: Article

Abstract

We present the first systematic physical modelling of the time-lag spectra between the soft (0.3–1 keV) and the hard (1.5–4 keV) X-ray energy bands, as a function of Fourier frequency, in a sample of 12 active galactic nuclei which have been observed by XMMNewton. We concentrate particularly on the negative X-ray time-lags (typically seen above 10-4 Hz), i.e. soft-band variations lag the hard-band variations, and we assume that they are produced by reprocessing and reflection by the accretion disc within a lamp-post X-ray source geometry. We also assume that the response of the accretion disc, in the soft X-ray bands, is adequately described by the response in the neutral Fe Kα line at 6.4 keV for which we use fully general relativistic ray-tracing simulations to determine its time evolution. These response functions, and thus the corresponding time-lag spectra, yield much more realistic results than the commonly used, but erroneous, top-hat models. Additionally, we parametrize the positive part of the time-lag spectra (typically seen below 10-4 Hz) by a power law. We find that the best-fitting black hole (BH) masses, M, agree quite well with those derived by other methods, thus providing us with a new tool for BH mass determination. We find no evidence for any correlation between M and the BH spin parameter, α, the viewing angle, θ, or the height of the X-ray source above the disc, h. Also on average, the X-ray source lies only around 3.7 gravitational radii above the accretion disc and θ is distributed uniformly between 20° and 60°. Finally, there is a tentative indication that the distribution of α may be bimodal above and below 0.62.

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Accepted/In Press date: 4 February 2014
e-pub ahead of print date: 3 March 2014
Published date: 21 April 2014
Keywords: accretion, accretion discs, black hole physics, relativistic processes, galaxies: active, galaxies: nuclei, x-rays: galaxies
Organisations: Astronomy Group

Identifiers

Local EPrints ID: 393518
URI: http://eprints.soton.ac.uk/id/eprint/393518
ISSN: 1365-2966
PURE UUID: 2c71e05e-6a92-469c-ad2a-d7446d20d3d1
ORCID for D. Emmanoulopoulos: ORCID iD orcid.org/0000-0002-3335-2446

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Date deposited: 27 Apr 2016 14:36
Last modified: 15 Mar 2024 00:02

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Contributors

Author: D. Emmanoulopoulos ORCID iD
Author: I.E. Papadakis
Author: M. Dovciak
Author: I. Mchardy

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