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dc.contributor.authorRiffel, Rogemar Andrépt_BR
dc.contributor.authorStorchi-Bergmann, Thaisapt_BR
dc.contributor.authorRiffel, Rogériopt_BR
dc.contributor.authorBianchin, Marinapt_BR
dc.contributor.authorZakamska, Nadia L.pt_BR
dc.contributor.authorDutra, Daniel Ruschelpt_BR
dc.contributor.authorSchönell Júnior, Astor Joãopt_BR
dc.contributor.authorRosario, Davidpt_BR
dc.contributor.authorRodriguez-Ardila, Albertopt_BR
dc.contributor.authorFischer, Travis C.pt_BR
dc.contributor.authorDavies, Richard I.pt_BR
dc.contributor.authorDametto, Natacha Zanonpt_BR
dc.contributor.authorHahn, Luis Gabriel Dahmerpt_BR
dc.contributor.authorCrenshaw, Daniel Michaelpt_BR
dc.contributor.authorBurtscher, Leonardpt_BR
dc.contributor.authorBentz, Misty Cheriept_BR
dc.date.accessioned2021-12-17T04:30:18Zpt_BR
dc.date.issued2021pt_BR
dc.identifier.issn0035-8711pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/233042pt_BR
dc.description.abstractWe use the Gemini NIFS instrument to map the H22.1218μm and Brγ flux distributions in the inner 0.04–2 kpc of a sample of 36 nearby active galaxies (0.001 ≲ z ≲ 0.056) at spatial resolutions from 4 to 250 pc. We find extended emission in 34 galaxies. In ∼55 per cent of them, the emission in both lines is most extended along the galaxy major axis, while in the other 45 per cent the extent follows a distinct orientation. The emission of H2 is less concentrated than that of Brγ, presenting a radius that contains half of the flux 60 per cent greater, on average. The H2 emission is driven by thermal processes – X-ray heating and shocks – at most locations for all galaxies, where 0.4<H2/Brγ<6⁠. For regions where H2/Brγ > 6 (seen in 40 per cent of the galaxies), shocks are the main H2 excitation mechanism, while in regions with H2/Brγ < 0.4 (25 per cent of the sample) the H2 emission is produced by fluorescence. The only difference we found between type 1 and type 2 active galactic nucleus (AGN) was in the nuclear emission-line equivalent widths that are smaller in type 1 than in type 2 due to a larger contribution to the continuum from the hot dusty torus in the former. The gas masses in the inner 125 pc radius are in the range 101−104 M⊙ for the hot H2 and 103−106 M⊙ for the ionized gas and would be enough to power the AGN in our sample for 105−108 yr at their current accretion rates.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofMonthly notices of the royal astronomical society. Oxford. Vol. 504, no. 3 (July 2021), p. 3265–3283pt_BR
dc.rightsOpen Accessen
dc.subjectEspectroscopiapt_BR
dc.subjectTechniques: imaging spectroscopyen
dc.subjectGalaxies: activeen
dc.subjectGaláxias ativaspt_BR
dc.subjectGalaxies: ISMen
dc.subjectMeio interestelarpt_BR
dc.subjectGalaxias seyfertpt_BR
dc.subjectGalaxies: Seyferten
dc.subjectFormacao de estrelaspt_BR
dc.titleThe AGNIFS survey : distribution and excitation of the hot molecular and ionized gas in the inner kpc of nearby AGN hostspt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001128211pt_BR
dc.type.originEstrangeiropt_BR


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