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dc.contributor.authorFinlez, Carolinapt_BR
dc.contributor.authorNagar, Neil M.pt_BR
dc.contributor.authorStorchi-Bergmann, Thaisapt_BR
dc.contributor.authorMüller, Allan Schnorrpt_BR
dc.contributor.authorRiffel, Rogemar Andrépt_BR
dc.contributor.authorLena, Davidept_BR
dc.contributor.authorMundell, Carole G.pt_BR
dc.contributor.authorElvis, Martinpt_BR
dc.date.accessioned2018-11-22T02:48:45Zpt_BR
dc.date.issued2018pt_BR
dc.identifier.issn0035-8711pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/184923pt_BR
dc.description.abstractNGC 3393, a nearby Seyfert 2 galaxy with nuclear radio jets, large-scale and nuclear bars, and a posited secondary supermassive black hole, provides an interesting laboratory to test the physics of inflows and outflows. Here we present and analyse the molecular gas [ALMA observations of CO J:2-1 emission over a field of view (FOV) of 45 arcsec × 45 arcsec, at 0. 56 (143 pc) spatial and 5 kms−1 spectral resolution), ionized gas and stars (GEMINI–GMOS/IFU; over an FOV of 4 arcsec × 5 arcsec, at 0. 62 (159 pc) spatial and 23 km s−1 spectral resolution) in NGC 3393. The ionized gas emission, detected over the complete GEMINI–GMOS FOV, has three identifiable kinematic components. A narrow (σ < 115 km s−1) component present in the complete FOV, which is consistent with rotation in the galaxy disc. A broad (σ > 115 km s−1) redshifted component, detected near the NE and SW radio lobes; which we interpret as a radio jet-driven outflow. And a broad (σ > 115 km s−1) blueshifted component that shows high velocities in a region perpendicular to the radio jet axis; we interpret this as an equatorial outflow. The CO J:2-1 emission is detected in spiral arms on 5–20 arcsec scales, and in two disturbed circumnuclear regions. The molecular kinematics in the spiral arms can be explained by rotation. The highly disturbed kinematics of the inner region can be explained by perturbations induced by the nuclear bar and interactions with the large scale bar. We find no evidence for, but cannot strongly rule out, the presence of the posited secondary black hole.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofMonthly notices of the royal astronomical society. Oxford. Vol. 479, no. 3 (Sept. 2018), p. 3892–3908pt_BR
dc.rightsOpen Accessen
dc.subjectGalaxias seyfertpt_BR
dc.subjectBlack hole physicsen
dc.subjectGaláxia NGC 3393pt_BR
dc.subjectGalaxies activeen
dc.subjectGalaxies individual (NGC 3393)en
dc.subjectCinemáticapt_BR
dc.subjectGalaxies kinematics and dynamicsen
dc.subjectBuracos negrospt_BR
dc.subjectGalaxies nucleien
dc.subjectGas ionizadopt_BR
dc.subjectGalaxies Seyferten
dc.titleThe complex jet- and bar- perturbed kinematics in NGC 3393 as revealed with ALMA and GEMINI–GMOS/IFUpt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001081519pt_BR
dc.type.originEstrangeiropt_BR


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