20 research outputs found

    Simultaneous spectral and reverberation modelling of relativistic reflection in Mrk 335

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    We present an X-ray spectral and timing model to investigate the broad and variable iron line seen in the high flux state of Mrk 335. The model consists of a variable X-ray source positioned along the rotation axis of the black hole that illuminates the accretion disc producing a back-scattered, ionized reflection spectrum. We compute time lags including full dilution effects and perform simultaneous fitting of the 2-10 keV spectrum and the frequency-dependent time lags of 2.5-4 vs. 4-6.5 keV bands. The best-fitting parameters are consistent with a black hole mass of approximately 1.3 x 10^7 M_sun, disc inclination of 45 degrees and the photon index of the direct continuum of 2.4. The iron abundance is 0.5 and the ionization parameter is 10^3 erg cm / s at the innermost part of the disc and decreases further out. The X-ray source height is very small, approximately 2 r_g. Furthermore, we fit the Fe L lags simultaneously with the 0.3-10 keV spectrum. The key parameters are comparable to those previously obtained. We also report the differences below 2 keV using the xillver and reflionx models which could affect the interpretation of the soft excess. While simultaneously fitting spectroscopic and timing data can break the degeneracy between the source height and the black hole mass, we find that the measurements of the source height and the central mass significantly depend on the ionization state of the disc and are possibly model-dependent.Comment: 11 pages, 8 figures, accepted for publication in MNRA

    X-ray time lags in AGN: inverse-Compton scattering and spherical corona model

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    We develop a physically motivated, spherical corona model to investigate the frequency-dependent time lags in AGN. The model includes the effects of Compton up-scattering between the disc UV photons and coronal electrons, and the subsequent X-ray reverberation from the disc. The time lags are associated with the time required for multiple scatterings to boost UV photons up to soft and hard X-ray energies, and the light crossing time the photons take to reach the observer. This model can reproduce not only low-frequency hard and high-frequency soft lags, but also the clear bumps and wiggles in reverberation profiles which should explain the wavy-residuals currently observed in some AGN. Our model supports an anti-correlation between the optical depth and coronal temperatures. In case of an optically thin corona, time delays due to propagating fluctuations may be required to reproduce observed time lags. We fit the model to the lag-frequency data of 1H0707-495, Ark 564, NGC 4051 and IRAS 13224-3809 estimated using the minimal bias technique so that the observed lags here are highest-possible quality. We find their corona size is ~7-15 r_g having the constrained optical depth ~2-10. The coronal temperature is ~150-300 keV. Finally, we note that the reverberation wiggles may be signatures of repeating scatters inside the corona that control the distribution of X-ray sources.Comment: 15 pages, 10 figures, accepted for publication in MNRA

    Investigating scaling relations in X-ray reverberating AGN using symbolic regression

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    Symbolic regression (SR) is a regression analysis based on genetic algorithms to search for mathematical expressions that best fit a given data set, by allowing the expressions themselves to mutate. We use the SR to analyze the parameter relations of the X-ray reverberating Active Galactic Nuclei (AGN) where the soft Fe-L lags were observed by XMM-Newton. Firstly, we revisit the lag-mass scaling relations by using the SR to derive all possible mathematical expressions and test them in terms of accuracy, simplicity and robustness. We find that the correlation between the lags, Ο„\tau, and the black hole mass, MBHM_{\rm BH}, is certain, but the relation should be written in the form of log⁑(Ο„)=Ξ±+Ξ²(log⁑(MBH/MβŠ™))Ξ³\log ({\tau}) = \alpha + \beta (\log{(M_{\rm BH}/M_{\odot})})^{\gamma}, where 1≲γ≲21 \lesssim \gamma \lesssim 2. Moreover, incorporating more parameters such as the reflection fraction (RFRF) and the Eddington ratio (Ξ»Edd\lambda_{\rm Edd}) to the lag-mass scaling relation is made possible by the SR. It reveals that Ξ±\alpha, rather than being a constant, can be βˆ’2.15+0.02RF-2.15 + 0.02RF or 0.03(RF+Ξ»Edd)0.03(RF + \lambda_{\rm Edd}), with the fine-tuned different Ξ²\beta and Ξ³\gamma. These further support the relativistic disc-reflection framework in which such functional dependencies can be straightforwardly explained. Furthermore, we derive their host-galaxy mass, Mβˆ—M_{\ast}, by fitting the spectral energy distribution (SED). We find that the SR model supports a non-linear MBHM_{\rm BH}--Mβˆ—M_{\ast} relationship, while log⁑(MBH/Mβˆ—)\log (M_{\rm BH}/M_{\ast}) varies between βˆ’5.4-5.4 and βˆ’1.5-1.5, with an average value of βˆΌβˆ’3.7\sim -3.7. No significant correlation between Mβˆ—M_{\ast} and Ξ»Edd\lambda_{\rm Edd} is confirmed in these samples.Comment: 14 pages, 7 figures, 2 tables, accepted for publication in MNRA

    Coronal height constraint in IRAS 13224-3809 and 1H 0707-495 by the random forest regressor

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    We develop a random forest regressor (RFR) machine learning model to trace the coronal evolution in two highly variable active galactic nuclei (AGNs) IRAS 13224-3809 and 1H 0707-495 observed with XMM-Newton, by probing the X-ray reverberation features imprinted on their power spectral density (PSD) profiles. Simulated PSDs in the form of a power-law, with similar frequency range and bins to the observed data, are produced. Then, they are convolved with relativistic disc-response functions from a lamp-post source before being used to train and test the model to predict the coronal height. We remove some bins that are dominated by Poisson noise and find that the model can tolerate the frequency-bin removal up to ∼10\sim 10 bins to maintain a prediction accuracy of R2>0.9R^{2} > 0.9. The black hole mass and inclination should be fixed so that the accuracy in predicting the source height is still >0.9> 0.9. The accuracy also increases with the reflection fraction. The corona heights for both AGN are then predicted using the RFR model developed from the simulated PSDs whose frequency range and bins are specifically adjusted to match those from each individual observation. The model suggests that their corona varies between ∼ 5βˆ’18Β rg\sim~5 - 18~r_{\rm g}, with R2>0.9R^{2} > 0.9 for all observations. Such high accuracy can still be obtained if the difference between the true mass and the trained value is ≲10%\lesssim 10\%. Finally, the model supports the height-changing corona under the light-bending scenario where the height is correlated to source luminosity in both IRAS 13224-3809 and 1H 0707-495.Comment: 9 Figures, 1 Table, Accepted for publication in MNRA

    X-ray timing and spectral analysis of reverberating active galactic nuclei

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    Simultaneous spectral and reverberation modelling of relativistic reflection in Mrk 335

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    Predicting the black hole mass and correlations in X-ray reverberating AGNs using neural networks

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    We develop neural network models to predict the black hole mass using 22 reverberating AGN samples in the XMM-Newton archive. The model features include the fractional excess variance (FvarF_{\rm var}) in 2-10 keV band, Fe-K lag amplitude, 2-10 keV photon counts and redshift. We find that the prediction accuracy of the neural network model is significantly higher than what is obtained from the traditional linear regression method. Our predicted mass can be confined within Β±(2\pm (2-5) per cent of the true value, suggesting that the neural network technique is a promising and independent way to constrain the black hole mass. We also apply the model to 21 non-reverberating AGN to rule out their possibility to exhibit the lags (some have too small mass and FvarF_{\rm var}, while some have too large mass and FvarF_{\rm var} that contradict the FvarF_{\rm var}-lag-mass relation in reverberating AGN). We also simulate 3200 reverberating AGN samples using the multi-feature parameter space from the neural network model to investigate the global relations if the number of reverberating AGN increases. We find that the FvarF_{\rm var}-mass anti-correlation is likely stronger with increasing number of newly-discovered reverberating AGN. Contrarily, to maintain the lag-mass scaling relation, the tight anti-correlation between the lag and FvarF_{\rm var} must preserve. In an extreme case, the lag-mass correlation coefficient can significantly decrease and, if observed, may suggest the extended corona framework where their observed lags are more driven by the coronal property rather than geometry.Comment: 15 pages, 12 figures, 4 tables, accepted for publication in MNRA

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

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    X-ray reflection from an accretion disc produces characteristic emission lines allowing us to probe the innermost regions in AGN. We investigate these emission lines under a framework of Riemannian geometrical optics where the corona has a refractive index of nβ‰ 1n \neq 1. The empty space outside is a vacuum with n=1n = 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 nn. The choice of nn alters the null geodesics, producing the effect which is analogous to the light deflection. For the corona with n>1n > 1, the disc on the far side within the corona covers a larger area on the observer' 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 n1n 1 and n<1n < 1 could induce extra shifts in the blue wing (Ξ”gmax\Delta g_{max}) to higher and lower energy, respectively. These effects are more prominent when the inclination angle is ≳60∘\gtrsim 60^\circ and the corona extends to ≳5rg\gtrsim 5r_g. To obtain the deviation of the line shift of Ξ”gmax≳0.01\Delta g_{\rm max} \gtrsim 0.01, the difference between the refractive index of the corona and that of the empty space must be Ξ”n≳0.5\Delta n \gtrsim 0.5%. Finally, the lensing corona can influence the arrival time of photons that may affect the observed variability of these emission linesComment: 12 pages, 11 figures, accepted for publication in MNRA
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