We report the first direct X-ray evidence that an AGN is hidden in the center of IRAS12393+3520. An ASCA observation of this target unveiled a bright (0.5-10 keV luminosity 3.9 x 1E42 erg/s) and variable source, with minimum observed doubling/halving time scale comprised in the range 30-75 ks. A model composed by a simple power-law, with photon index ~ 1.8 and an absorption edge, whose threshold energy is consistent with K-shell photoionization of O VII, provides an adequate fit of the spectrum. This suggests that we are observing the emission from the nuclear region through a warm absorber of N_H ~ a few 1E21 per square cm. If it has internal dust with Galactic gas-to-dust ratio, it could explain the lack of broad Hβ emission, even in the episodic presence of a broad Hα emission line. Optical spectra obtained over several years show indeed variations in the strength of this broad Hα component. A distribution of dusty, optically thick matter on spatial scales a few hundreds parsec, which does not intercept the line of sight towards the nucleus, is probably required to account simultaneously for the relative [OIII] luminosity deficit in comparison to the X-rays. The high IR to X-ray luminosity ratio is most likely due to intense star formation in the circumnuclear region. IRAS12393+3520 might thus exhibit simultaneously nuclear activity and remarkable star formation.
A direct view of the AGN powering IRAS12393.3520
RAFANELLI, PIERO;
2000
Abstract
We report the first direct X-ray evidence that an AGN is hidden in the center of IRAS12393+3520. An ASCA observation of this target unveiled a bright (0.5-10 keV luminosity 3.9 x 1E42 erg/s) and variable source, with minimum observed doubling/halving time scale comprised in the range 30-75 ks. A model composed by a simple power-law, with photon index ~ 1.8 and an absorption edge, whose threshold energy is consistent with K-shell photoionization of O VII, provides an adequate fit of the spectrum. This suggests that we are observing the emission from the nuclear region through a warm absorber of N_H ~ a few 1E21 per square cm. If it has internal dust with Galactic gas-to-dust ratio, it could explain the lack of broad Hβ emission, even in the episodic presence of a broad Hα emission line. Optical spectra obtained over several years show indeed variations in the strength of this broad Hα component. A distribution of dusty, optically thick matter on spatial scales a few hundreds parsec, which does not intercept the line of sight towards the nucleus, is probably required to account simultaneously for the relative [OIII] luminosity deficit in comparison to the X-rays. The high IR to X-ray luminosity ratio is most likely due to intense star formation in the circumnuclear region. IRAS12393+3520 might thus exhibit simultaneously nuclear activity and remarkable star formation.Pubblicazioni consigliate
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