STScI Preprint #1253 PREV UP NEXT         INDEX SEARCH

STScI Preprint #1253


The Ionization Fraction in the Obscuring `Torus' of An Active Galactic Nucleus

Authors: A. S. Wilson 1,10, A. L. Roy 2, J. S. Ulvestad 2, E. J. M. Colbert3, K. A. Weaver 4, J. A. Braatz 5, C. Henkel 6, M. Matsuoka7, S. Xue 7, N. Iyomoto 8, K. Okada9
The LINER galaxy NGC 2639 contains a water vapor megamaser, suggesting the presence of an edge-on nuclear accretion disk or torus. This galaxy is thus a good candidate for revealing absorption by the torus of any compact nuclear continuum emission. In this paper, we report VLBA radio maps at three frequencies and an ASCA X-ray spectrum obtained to search for free-free and photoelectric absorptions, respectively. The radio observations reveal a compact (< 0.2 pc) nuclear source with a spectrum that turns over sharply near 5 GHz. This turnover may reflect either synchrotron self-absorption or free-free absorption. The galaxy is detected by ASCA with an observed luminosity of 1.4 × 1041 erg s-1 in the 0.6-10 keV band. The X-ray spectrum shows emission in excess of a power-law model at energies greater than 4 keV; we interpret this excess as compact, nuclear, hard X-ray emission with the lower energies photoelectrically absorbed by an equivalent hydrogen column of ~5×1023 cm-2. If we assume that the turnover in the radio spectrum is caused by free-free absorption and that both the free-free and photoelectric absorptions are produced by the same gaseous component, the ratio int ne2 dl/int nH dl may be determined. If the masing molecular gas is responsible for both absorptions, the required ionization fraction is >~ 1.3 × 10-5, which is comparable to the theoretical upper limit derived by Neufeld, Maloney & Conger (1994) for X-ray heated molecular gas. The two values may be reconciled if the molecular gas is very dense nH2 >~109 cm-3. The measured ionization fraction is also consistent with the idea that both absorptions occur in a hot (~6,000 K), weakly ionized (ionization fraction a few times 10-2) atomic region that may co-exist with the warm molecular gas. If this is the case, the absorbing gas is ~1 pc from the nucleus. We rule out the possibility that both absorptions occur in a fully ionized gas near 104 K. If our line of sight passes through more than one phase, the atomic gas probably dominates the free-free absorption while the molecular gas may dominate the photoelectric absorption.
Status:
Appeared in: The Astrophysical Journal, 505:587-593, 1998

Affiliations:
1) Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218
2) National Radio Astronomy Observatory, P. O. Box 0, Socorro, NM 87801
3) Mail Code 662, Laboratory for High Energy Astrophysics, NASA Goddard Space Flight Center, Greenbelt, MD 20771
4) The Johns Hopkins University, Department of Physics and Astronomy, Baltimore, MD 21218
5) National Radio Astronomy Observatory, P. O. Box 2, Green Bank, WV 24944
6) Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, D-53121 Bonn, Germany
7) The Institute of Physical and Chemical Research (RIKEN), 2-1, Hirosawa, Wako-shi, Saitama 351-01, Japan
8) Department of Physics, University of Tokyo, 3-1, Hongo 7-chome, Bunkyo-ku, Tokyo 113, Japan
9) Institute of Space and Astronautical Science, 3-1-1, Yoshinodai, Sagamihara, Kanagawa 229, Japan
10) Also Astronomy Department, University of Maryland, College Park, MD 20742
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Last updated, June 5, 1998