The extended narrow-line region of the Seyfert 1 galaxy ESO 362-G18 versus that of the Seyfert 2 galaxy ESO 362-G8

• Autor(a) principal: Fraquelli, Henrique Aita
• Data de Publicação: 2000
• Outros Autores: Storchi-Bergmann, Thaisa, Binette, Luc
• Tipo de documento: Artigo
• Idioma: eng
• Título da fonte: Repositório Institucional da UFRGS
• Texto Completo: http://hdl.handle.net/10183/108874
• topic: Galaxias seyfert; Nucleo galatico; Galáxias ativas; Formacao de estrelas; Espectros astronômicos; Materia interestelar; Luminosidade; Galaxies : active; Galaxies : ISM; Galaxies : nuclei; Galaxies : seyfert

We use long-slit spectroscopic data to study in detail the extended narrow-line regions (ENLRs) of the Seyfert 1 galaxy ESO 362-G18 and Seyfert 2 galaxy ESO 362-G8. These two galaxies have similar emission-line luminosities and extents of the ENLR (~4 kpc), whose shapes in previous narrowband [O III] images suggest anisotropic escape of the nuclear ionizing radiation as expected for shadowing by a nuclear torus in the framework of the unified model. In the Seyfert 1 galaxy the high-excitation gas shows an approximately cone-shaped morphology. From the observed kinematics, we conclude that the gas within the cone most probably belongs to the galaxy disk, which implies that the collimation axis is closer to the disk than half the opening angle of the cone of ionizing radiation. In the Seyfert 2 galaxy, the main structure in the high-excitation gas is an emission blob which apparently consists of a highlatitude cloud being blown away from the nuclear region and ionized by the nuclear source. We use the radial distribution of stellar population features in order to extrapolate this population to the nucleus and isolate the optical continuum of the nuclear source. We obtain a featureless power-law continuum F v ∝ v -0.76 for the Seyfert 1 galaxy, while for the Seyfert 2 galaxy we conclude that the lPl~0.76 nuclear bluer color and smaller equivalent widths of the absorption lines are due to an aging burst of star formation (age≈300 Myr) and that the nuclear source is hidden from direct view. Using the photoionization code MAPPINGS Ic and a mixture of matter-bounded (MB) and ionization-bounded (IB) clouds, we model the ENLRs of the two galaxies. We use all the observables, mostly the emission-line fluxes as a function of distance from the nucleus and the optical nuclear continuum observed in the Seyfert 1 galaxy as well as its X-ray flux, to constrain the parameters of a self consistent model for the ENLR. For both galaxies, we conclude that a power-law ionizing continuum F v ∝ v -1.2 better reproduces the high-excitation lines near the nucleus than a multisegmented power law used in previous works. For the Seyfert 1 galaxy ESO 362-G18, the inferred luminosity of the ionizing continuum can be reconciled with the flux observed in the optical, while in the X-rays the observed flux is ~100 times weaker than that necessary to reproduce the line fluxes, suggesting that the X-ray continuum is absorbed toward Earth. For the Seyfert 2 galaxy ESO 362-G8, the inferred ionizing continuum when extrapolated to the optical implies a minimum obscuration toward the nuclear source of AV≈4.0 mag. In the hypothesis of an isotropic nuclear source, in order to better constrain the model parameters, we have adopted symmetrical physical conditions as a function of distance on both sides of the nucleus : namely, the ionizing flux, the temperature, density, and ionization parameter of the MB gas, and the metallicity. The radial density behavior of the IB gas was observationally inferred from the [S II] doublet ratio. The only free parameter, which was allowed to vary independently, was the relative proportion of the MB and IB emission-line components along the ENLR. The high-excitation gas within the cone of ESO 362-G18 and within the blob of ESO 362-G8 have been modeled as regions of larger mass contribution from the MB component relative to other locations of the ENLR. We derive the filling factors, covering factors, and gas masses along the ENLR as a function of distance from the nucleus. A comparison between the model results for the two galaxies shows that, around the nucleus, the Seyfert 1 galaxy has a larger excitation due to a larger contribution of the MB component. However, in the cone, the excitation is lower than in the blob of the Seyfert 2 galaxy due to a combination of a lower ionizing Ñux and larger gas density in the disk of the Seyfert 1 galaxy. The total ionized gas mass derived for the blob in the Seyfert 2 galaxy is 10 5.8 Mʘ, consistent with its proposed origin in a nuclear superwind which probably occurred ~300 Myr ago, while the ionized gas mass inthe disk of the Seyfert 1 galaxy is 1 order of magnitude smaller.