4.7 Article

Implications of the Warm Corona and Relativistic Reflection Models for the Soft Excess in Mrk 509

Journal

ASTROPHYSICAL JOURNAL
Volume 871, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/aaf739

Keywords

accretion, accretion disks; black hole physics; galaxies: active; galaxies: individual (Mrk 509); galaxies: nuclei

Funding

  1. NASA [NNX15AV31G, 80NSSC177K0515, PF5-160144, NNX15AP24G, NNG08FD60C]
  2. Alexander von Humboldt Foundation
  3. black hole initiative at Harvard University - John Templeton Foundation
  4. Programma per Giovani Ricercatori-anno 2014 Rita Levi Montalcini
  5. CONICYT+PAI Convocatoria Nacional subvencion a instalacion en la academia convocatoria ano [2017 PAI77170080]
  6. National Aeronautics and Space Administration
  7. STFC [ST/N004027/1] Funding Source: UKRI
  8. NASA [NNX15AP24G, 797490, NNX15AV31G, 800510] Funding Source: Federal RePORTER

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We present the analysis of the first Nuclear Spectroscopic Telescope Array observations (similar to 220 ks), simultaneous with the last Suzaku observations (similar to 50 ks), of the active galactic nucleus of the bright Seyfert 1 galaxy Mrk 509. The time-averaged spectrum in the 1-79 keV X-ray band is dominated by a power-law continuum (Gamma similar to 1.8-1.9), a strong soft excess around 1 keV, and signatures of X-ray reflection in the form of Fe K emission (similar to 6.4 keV), an Fe K absorption edge (similar to 7.1 keV), and a Compton hump due to electron scattering (similar to 20-30 keV). We show that these data can be described by two very different prescriptions for the soft excess: a warm (kT similar to 0.5-1 keV) and optically thick (tau similar to 10-20) Comptonizing corona or a relativistically blurred ionized reflection spectrum from the inner regions of the accretion disk. While these two scenarios cannot be distinguished based on their fit statistics, we argue that the parameters required by the warm corona model are physically incompatible with the conditions of standard coronae. Detailed photoionization calculations show that even in the most favorable conditions, the warm corona should produce strong absorption in the observed spectrum. On the other hand, while the relativistic reflection model provides a satisfactory description of the data, it also requires extreme parameters, such as maximum black hole spin, a very low and compact hot corona, and a very high density for the inner accretion disk. Deeper observations of this source are thus necessary to confirm the presence of relativistic reflection and further understand the nature of its soft excess.

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