{"id":533,"date":"2020-01-09T22:47:05","date_gmt":"2020-01-09T22:47:05","guid":{"rendered":"http:\/\/itziararetxaga.net\/2020\/01\/modelling-the-strongest-silicate-emission-features-of-local-type-1-agn\/"},"modified":"2020-01-23T16:06:52","modified_gmt":"2020-01-23T16:06:52","slug":"modelling-the-strongest-silicate-emission-features-of-local-type-1-agn","status":"publish","type":"post","link":"http:\/\/www.itziararetxaga.net\/eu\/2020\/01\/modelling-the-strongest-silicate-emission-features-of-local-type-1-agn\/","title":{"rendered":"Modelling the strongest silicate emission features of local type 1 AGN"},"content":{"rendered":"

Mart\u00ednez-Paredes, M.<\/a>; Gonz\u00e1lez-Mart\u00edn, O.<\/a>; Esparza-Arredondo, D.<\/a>; Kim, M.<\/a>; Alonso-Herrero, A.<\/a>; Krongold, Y.<\/a>; Hoang, T.<\/a>; Ramos Almeida, C.<\/a>; Aretxaga, I.<\/a>; Dultzin, D.<\/a>; Hodgson, J.<\/a><\/p>\n

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Accepted for publication in Astrophysical Journal (arXiv: 2001.00844<\/a>)<\/p>\n

Abstract<\/h4>\n

We measure the 10 and 18<\/span>\u03bc<\/span><\/span><\/span><\/span>m silicate features in a sample of 67 local (z<\/span><<\/span>0.1<\/span><\/span><\/span><\/span>) type 1 active galactic nuclei (AGN) with available Spitzer spectra dominated by non-stellar processes. We find that the 10<\/span>\u03bc<\/span><\/span><\/span><\/span>m silicate feature peaks at 10.3<\/span>+<\/span>0.7<\/span><\/span><\/span>\u2212<\/span>0.9<\/span><\/span><\/span><\/span>\u03bc<\/span><\/span><\/span><\/span>m with a strength (Si_p<\/span><\/span><\/span><\/span><\/span><\/span><\/span> = ln f_p<\/span><\/span><\/span><\/span><\/span><\/span><\/span>(spectrum)\/f_p<\/span><\/span><\/span><\/span><\/span><\/span><\/span>(continuum)) of 0.11<\/span>+<\/span>0.15<\/span><\/span><\/span>\u2212<\/span>0.36<\/span><\/span><\/span><\/span><\/span><\/span><\/span>, while the 18<\/span>\u03bc<\/span><\/span><\/span><\/span>m one peaks at 17.3<\/span>+<\/span>0.4<\/span><\/span><\/span>\u2212<\/span>0.7<\/span><\/span><\/span><\/span>\u03bc<\/span><\/span><\/span><\/span>m with a strength of 0.14<\/span>+<\/span>0.06<\/span><\/span><\/span>\u2212<\/span>0.06<\/span><\/span><\/span><\/span><\/span><\/span><\/span>. We select from this sample sources with the strongest 10\u03bc<\/span><\/span><\/span><\/span>m silicate strength (\u03c3_<\/span>S<\/span>i<\/span>10<\/span>\u03bc<\/span>m<\/span><\/span><\/span><\/span><\/span><\/span><\/span>><\/span>0.28<\/span><\/span><\/span><\/span>, 10 objects). We carry out a detailed modeling of the IRS\/ Spitzer spectra by comparing several models that assume different geometries and dust composition: a smooth torus model, two clumpy torus models, a two-phase medium torus model, and a disk+outflow clumpy model. We find that the silicate features are well modeled by the clumpy model of Nenkova et al. 2008, and among all models those including outflows and complex dust composition are the best (Hoenig et al. 2017). We note that even in AGN-dominated galaxies it is usually necessary to add stellar contributions to reproduce the emission at the shortest wavelengths.<\/p>\n

\"Si
Silicate strength of the 10 and 18um silicate features. Grey circles represent the values measured in the models, while the stars are the measurements obtained from the AGN-dominated IRS\/Spitzer spectra of the Si-s sample. The colours of the stars indicate different range of bolometric luminosities. (Fig 6).<\/figcaption><\/figure>\n<\/div>\n