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dc.contributor.authorSales, Dinalva Aires dept_BR
dc.contributor.authorRobinson, Andrewpt_BR
dc.contributor.authorAxon, David J.pt_BR
dc.contributor.authorGallimore, Jack F.pt_BR
dc.contributor.authorKharb, Preetipt_BR
dc.contributor.authorCurran, R. L.pt_BR
dc.contributor.authorO'Dea, Christopher Peterpt_BR
dc.contributor.authorBaum, Stefi Alisonpt_BR
dc.contributor.authorElitzur, Moshept_BR
dc.contributor.authorMittal, Rupalpt_BR
dc.date.accessioned2015-05-15T02:01:57Zpt_BR
dc.date.issued2015pt_BR
dc.identifier.issn0004-637Xpt_BR
dc.identifier.urihttp://hdl.handle.net/10183/116375pt_BR
dc.description.abstractWe present a multiwavelength study of the OH megamaser galaxy IRAS16399−0937, based on new Hubble Space Telescope (HST)/Advanced Camera for Surveys F814W and Hα+[N ii] images and archive data from HST, Two Micron All Sky Survey, Spitzer, Herschel and the Very Large Array. This system has a double nucleus, whose northern (IRAS16399N) and southern (IRAS16399S) components have a projected separation of ∼6"(3.4 kpc) and have previously been identified based on optical spectra as a low ionization nuclear emission line region (LINER) and starburst nucleus, respectively. The nuclei are embedded in a tidally distorted common envelope, in which star formation is mostly heavily obscured. The infrared spectrum is dominated by strong polycyclic aromatic hydrocarbon, but deep silicate and molecular absorption features are also present, and are strongest in the IRAS16399N nucleus. The 0.435–500 μm spectral energy distribution was fitted with a model including stellar, interstellar medium and active galactic nucleus (AGN) torus components using our newMarkov ChainMonte Carlo code, clumpyDREAM. The results indicate that the IRAS16399N contains an AGN (Lbol ∼ 1044 erg s-ˡ) deeply embedded in a quasi-spherical distribution of optically thick clumps with a covering fraction ≈1. We suggest that these clumps are the source of the OHM emission in IRAS16399−0937. The high torus covering fraction precludes AGN photoionization as the origin of the LINER spectrum, however, the spectrum is consistent with shocks (v ∼ 100–200 km s-ˡ). We infer that the ∼108Mʘ black hole in IRAS16399N is accreting at a small fraction (∼1%) of its Eddington rate. The low accretion rate and modest nuclear star formation rates suggest that while the gas-rich major merger forming the IRAS16399−0937 system has triggered widespread star formation, the massive gas inflows expected from merger simulations have not yet fully developed.en
dc.format.mimetypeapplication/pdf
dc.language.isoengpt_BR
dc.relation.ispartofThe astrophysical journal. Bristol. Vol. 799, no. 1 (Jan. 2015), 25, 28 p.pt_BR
dc.rightsOpen Accessen
dc.subjectGalaxies: activeen
dc.subjectGaláxias ativaspt_BR
dc.subjectGalaxies: individual (IRAS16399–0937, IRASF16399–0937)en
dc.subjectMateria interestelarpt_BR
dc.subjectNucleo galaticopt_BR
dc.subjectGalaxies: interactionsen
dc.subjectFormacao de estrelaspt_BR
dc.subjectGalaxies: irregularen
dc.subjectAcreçãopt_BR
dc.subjectGalaxies: ISMen
dc.subjectGalaxies: starbursten
dc.subjectBuracos negrospt_BR
dc.subjectFotoionizacaopt_BR
dc.subjectInfrared: galaxiesen
dc.subjectCompostos orgânicospt_BR
dc.subjectRadio continuum: galaxiesen
dc.subjectEspectros infravermelhospt_BR
dc.subjectEspectros astronômicospt_BR
dc.titleAn embedded active nucleus in the OH megamaser galaxy IRAS16399-0937pt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000965519pt_BR
dc.type.originEstrangeiropt_BR


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