Abstract
We develop the power spectral density (PSD) model to explain the nature of the X-ray variability in IRAS 13224–3809, including the full effects of the X-ray reverberation due to the lamppost source. We utilize 16 XMM-Newton observations individually as well as group them into three different luminosity bins: low, medium, and high. The soft (0.3–1 keV) and hard (1.2–5 keV) PSD spectra are extracted and simultaneously fitted with the model. We find that the corona height changes from h ∼ 3 rg during the lowest luminosity state to ∼25 rg during the highest luminosity state. This provides further evidence that the source height from the reverberation data is significantly larger than what is constrained by the spectral analysis. Furthermore, as the corona height increases, the energy spectrum tends to be softer while the observed fractional excess variance, Fvar, reduces. We find that the PSD normalization is strongly correlated with Fvar and moderately correlated with the PSD bending index. Therefore, the normalization is dependent on the accretion rate that controls the intrinsic shape of the PSD. While the intrinsic variability of the disk is manifested by the reverberation signals, the disk and corona may evolve independently. Our results suggest that, as the source height increases, the disk itself generates less overall variability power but more high-frequency variability resulting in the PSD spectrum that flattens out (i.e., the inner disk becomes more active). Using the luminosity-bin data, the hint of the Lorentzian component is seen, with the peak appearing at lower frequencies with increasing luminosity.
| Original language | English |
|---|---|
| Article number | ac7d55 |
| Number of pages | 13 |
| Journal | Astrophysical Journal |
| Volume | 934 |
| Issue number | 2 |
| DOIs | |
| Publication status | Published - 4 Aug 2022 |
Bibliographical note
Funding Information:This work (grant No. RGNS 64–118) was supported by the Office of the Permanent Secretary, Ministry of Higher Education, Science, Research and Innovation (OPS MHESI), Thailand Science Research and Innovation (TSRI), and Suranaree University of Technology. P.C. thanks funding support from the NSRF via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation (grant number B16F640076). W.L. was supported in part by Srinakharinwirot University (grants no. 035/2565) and the National Astronomical Research Institute of Thailand (NARIT). J.J. acknowledges support from the Leverhulme Trust, the Isaac Newton Trust, and St Edmund’s College, University of Cambridge.
Publisher Copyright:
© 2022. The Author(s). Published by the American Astronomical Society.