1996A&A...314..393C


Query : 1996A&A...314..393C

1996A&A...314..393C - Astronomy and Astrophysics, volume 314393-413 (1996/10-2)

Quasi-spherical accretion of optically thin clouds as a model for the optical/UV/soft X-ray emission of AGN.

COLLIN-SOUFFRIN S., CZERNY B., DUMONT A.-M. and ZYCKI P.T.

Abstract (from CDS):

We examine four models for the optical/UV/soft X-ray emission of AGN: a mechanically heated plasma, either optically thin or thick for electron scattering, and a radiatively heated plasma, either optically thin or thick for electron scattering. We present detailed computations of the emitted spectra, and we discuss the total energy budget (including the requirement for the mass accretion flow), and the interaction with the hot optically thin medium responsible for hard X-ray emission. We show that in no case the spectrum can be considered as due to a pure free-free process: lines and/or free-bound continuum are always important. We can eliminate mechanical heating on the basis of variability time scales and of a detailed fit of the spectrum in the optical/UV/X-ray range. If the system of clouds is radiatively heated, the energy budget requires that it is optically thick to electron scattering. Finally, we conclude that a system of radiatively heated clouds, optically thick for electron scattering and having a covering factor close to unity, is a viable model for Seyfert galaxies. The same model is applicable for quasars although one cannot rule out in their case a small contribution from mechanical heating. Therefore we propose a new model for the emission of the optical to X-ray spectrum in AGN, made of a quasi-spherical (or a thick disk) distribution of mildly optically thick clouds. Smaller covering factor, 0.5-0.9, and smaller optical depth for electron scattering, ∼50, are more appropriate for Seyfert galaxies while larger values (>0.9 and ∼500 respectively) are deduced for quasars. As a consequence, we expect higher Eddington ratios in quasars than in Seyfert galaxies. One peculiarity of the model is that UV is due to pure emission, and X-rays to a combination of reflection and primary spectrum and that absorption features are weak in the X-ray range in spite of the large covering factor. Although it is attractive, this cloud scenario is not unique for the UV-X emission of AGN, with two others being: reprocessing clouds radiating as black bodies and accretion disks with hot coronae. We discuss the prospects of differentiation between these possibilities.

Abstract Copyright: ∼

Journal keyword(s): galaxies: active - galaxies: nuclei - radiation mechanisms: thermal - ultraviolet: galaxies - X-rays: galaxies

CDS comments: p. 404 IR 1334+243 = IRAS 13349+2438

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Z 232-3 Sy1 05 54 53.6080860768 +46 26 21.624853488   15.37 14.62     ~ 563 3
2 NGC 4151 Sy1 12 10 32.5759813872 +39 24 21.063527532   12.18 11.48     ~ 3938 2
3 IRAS 13349+2438 Sy1 13 37 18.7199358192 +24 23 03.319883484     15.0     ~ 410 0
4 IC 4329A Sy1 13 49 19.2601801224 -30 18 34.213815504   13.81 13.66 12.18 12.35 ~ 876 1
5 2MASS J21145258+0607423 Sy1 21 14 52.5774985320 +06 07 42.433198104   16.06 15.77     ~ 227 0
6 PKS J2158-3013 BLL 21 58 52.0652249880 -30 13 32.118447792   13.36 13.09 12.62   ~ 1829 1

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