TY - JOUR
T1 - The narrow Fe K α line and the molecular torus in active galactic nuclei
T2 - An IR/X-ray view
AU - Ricci, C.
AU - Ueda, Y.
AU - Ichikawa, K.
AU - Paltani, S.
AU - Boissay, R.
AU - Gandhi, P.
AU - Stalevski, M.
AU - Awaki, H.
PY - 2014/7
Y1 - 2014/7
N2 - The narrow component of the iron Kα is an almost ubiquitous feature in the X-ray spectra of active galactic nuclei (AGN) and is believed to originate in neutral material, possibly located in the molecular torus. This would imply a tight connection between the Fe Kα equivalent width (EW) and the physical properties of the torus. In a recent work we have shown that the decrease in the covering factor of the torus with the luminosity, as expected by luminosity-dependent unification models, would be able to explain the decrease in Fe Kα EW with the luminosity (i.e. the X-ray Baldwin effect). Recent developments in the study of the mid-IR (MIR) spectrum of AGN allow important parameters of the torus to be deduced, such as its covering factor (f obs) and equatorial column density (NHT), by applying clumpy torus models. Using XMM-Newton/EPIC observations of a sample of 24 type-I AGN, we investigate the relation between the physical parameters of the torus obtained by recent MIR works and the properties of the Fe Kα line. We correct the values of the Fe Kα EW by taking the inclination angle, the photon index, the equatorial column density, and half-opening angle of the torus into account using a physical torus model of X-ray reprocessed radiation. We find that the relation between Fe Kα EW and fobs shows a slope that is consistent with the expected value, albeit with low statistical significance. A trend that is consistent with the theoretical prediction is also found when comparing the Fe Kα EW to NH T. Our work seems to confirm that the bulk of the narrow Fe Kα line is produced by the same material responsible for the MIR emission.
AB - The narrow component of the iron Kα is an almost ubiquitous feature in the X-ray spectra of active galactic nuclei (AGN) and is believed to originate in neutral material, possibly located in the molecular torus. This would imply a tight connection between the Fe Kα equivalent width (EW) and the physical properties of the torus. In a recent work we have shown that the decrease in the covering factor of the torus with the luminosity, as expected by luminosity-dependent unification models, would be able to explain the decrease in Fe Kα EW with the luminosity (i.e. the X-ray Baldwin effect). Recent developments in the study of the mid-IR (MIR) spectrum of AGN allow important parameters of the torus to be deduced, such as its covering factor (f obs) and equatorial column density (NHT), by applying clumpy torus models. Using XMM-Newton/EPIC observations of a sample of 24 type-I AGN, we investigate the relation between the physical parameters of the torus obtained by recent MIR works and the properties of the Fe Kα line. We correct the values of the Fe Kα EW by taking the inclination angle, the photon index, the equatorial column density, and half-opening angle of the torus into account using a physical torus model of X-ray reprocessed radiation. We find that the relation between Fe Kα EW and fobs shows a slope that is consistent with the expected value, albeit with low statistical significance. A trend that is consistent with the theoretical prediction is also found when comparing the Fe Kα EW to NH T. Our work seems to confirm that the bulk of the narrow Fe Kα line is produced by the same material responsible for the MIR emission.
KW - Galaxies: Seyfert
KW - Galaxies: active
KW - Infrared: galaxies
KW - Quasars: emission lines
KW - Quasars: general
KW - X-rays: galaxies
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U2 - 10.1051/0004-6361/201322701
DO - 10.1051/0004-6361/201322701
M3 - Article
AN - SCOPUS:84905229622
SN - 0004-6361
VL - 567
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
M1 - A142
ER -