2.5-11 micron spectroscopy and imaging of AGNs: implication for unification schemes

TL;DR

This study uses 2.5-11 micron spectroscopy and imaging to compare Seyfert 1 and Seyfert 2 galaxies, supporting unification models by revealing differences in MIR continuum and PAH features related to viewing angles and obscuration.

Contribution

It provides new MIR spectroscopic evidence for the unification scheme of AGNs, quantifying extinction and spatially constraining the torus and reflecting regions.

Findings

Sf1 have strong power-law MIR continuum and weak PAH emission.

Sf2s show weak continuum but strong PAH features, indicating higher obscuration.

PAH emission is from bulge ISM, unrelated to nuclear activity.

Abstract

We present 2.5-11 micron spectrophotometric & imaging ISO observations of 28 Sf1, 29 Sf2 & 1 normal galaxy. The Sf1 & Sf2 MIR spectra are statistically different: Sf1 have a strong power-law continuum of index -0.84+/-0.24 & weak PAH emission bands. Sf2s have a weak continuum & very strong PAH emission features with EW (equivalent widths) up to 7.2 micron. On the other hand, the Sf1 and Sf2 PAH luminosities do not differ statistically and the 7 micron continuum is ~8 times less luminous in Sf2s than in Sf1s. The PAH emission is unrelated to the nuclear activity & arises in the bulge ISM. PAH EW are thus a sensitive nuclear redenning indicator. These results are consistent with unified schemes & imply that the Sf2 MIR nuclear continuum is, on the average, extinguished by 92+/-37 visual magnitudes whereas it is directly visible in Sf1s. The dispersion in Sf2's PAH EW is consistent with the expected spread in viewing angles. Those Sf2s with PAH EW > 5 micron suffer from > 125 magnitudes of extinction and are invariably weak X-ray sources. Such Sf2s represent the highly inclined objects where our line of sight intercepts the full extent of the torus. About 1/3rd of the Sf2s have PAH EW <= 2 micron, in the range of Sf1s. Among them, those which have been observed in spectropolarimetry or IR spectroscopy invariably display "hidden" broad lines. As proposed by Heisler et al (1997), such Sf2s are most likely seen at grazing incidence such that one has a direct view of both the "reflecting screen" and the torus inner wall emitting the MIR continuum. Our observations thus constrain the screen & the torus inner wall to be spatially co-located. Finally, the 9.7 micron Silicate feature appears weakly in emission in Sf1s, implying that the torus vertical thickness cannot significantly exceed E+24 cm-2