Feruglio, ChiaraChiaraFeruglioFiore, F.F.FioreCarniani, S.S.CarnianiMaiolino, R.R.MaiolinoD'ODORICO, ValentinaValentinaD'ODORICOLuminari, A.A.LuminariBarai, P.P.BaraiBischetti, M.M.BischettiBONGIORNO, ANGELAANGELABONGIORNOCRISTIANI, StefanoStefanoCRISTIANIFerrara, A.A.FerraraGallerani, S.S.GalleraniMarconi, AlessandroAlessandroMarconiPallottini, A.A.PallottiniPiconcelli, E.E.PiconcelliZAPPACOSTA, LucaLucaZAPPACOSTA2020-10-192020-10-1920180004-6361http://hdl.handle.net/20.500.12386/27890We present ALMA observations of the CO(6-5) and [CII] emission lines and the sub-millimeter continuum of the z ∼ 6 quasi-stellar object (QSO) SDSS J231038.88+185519.7. Compared to previous studies, we have analyzed a synthetic beam that is ten times smaller in angular size, we have achieved ten times better sensitivity in the CO(6-5) line, and two and half times better sensitivity in the [CII] line, enabling us to resolve the molecular gas emission. We obtain a size of the dense molecular gas of 2.9 ± 0.5 kpc, and of 1.4 ± 0.2 kpc for the 91.5 GHz dust continuum. By assuming that CO(6-5) is thermalized, and by adopting a CO to H<SUB>2</SUB> conversion factor α<SUB>CO</SUB> = 0.8 M<SUB>☉</SUB>K<SUP>-1</SUP> (km s)<SUP>-1</SUP> pc<SUP>2</SUP>, we infer a molecular gas mass of M(H<SUB>2</SUB>) = (3.2±0.2)×10<SUP>10</SUP> M<SUB>☉</SUB>. Assuming that the observed CO velocity gradient is due to an inclined rotating disk, we derive a dynamical mass of M<SUB>dyn</SUB>sin<SUP>2</SUP>(i)=(2.4 ± 0.5)×10<SUP>10</SUP> M<SUB>☉</SUB>, which is a factor of approximately two smaller than the previously reported estimate based on [CII]. Regarding the central black hole, we provide a new estimate of the black hole mass based on the C IV emission line detected in the VLT/X-shooter spectrum: M<SUB>BH</SUB> = (1.8 ± 0.5)×10<SUP>9</SUP> M<SUB>☉</SUB>. We find a molecular gas fraction of μ = M(H<SUB>2</SUB>)/M<SUP>*</SUP> ∼ 4.4, where M<SUP>∗</SUP> ≈ M<SUB>dyn</SUB> - M(H<SUB>2</SUB>) - M(BH). We derive a ratio ν<SUB>rot</SUB>/σ ≈ 1 - 2 suggesting high gas turbulence, outflows/inflows and/or complex kinematics due to a merger event. We estimate a global Toomre parameter Q ∼ 0.2 - 0.5, indicating likely cloud fragmentation. We compare, at the same angular resolution, the CO(6-5) and [CII] distributions, finding that dense molecular gas is more centrally concentrated with respect to [CII]. We find that the current BH growth rate is similar to that of its host galaxy. <P />The reduced data cubes and images are only available at the CDS via anonymous ftp to <A href="http://cdsarc.u-strasbg.fr/">http://cdsarc.u-strasbg.fr</A> (ftp://130.79.128.5) or via <A href="http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/619/A39">http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/619/A39STAMPAenThe dense molecular gas in the z ∼ 6 QSO SDSS J231038.88+185519.7 resolved by ALMAArticle10.1051/0004-6361/2018331742-s2.0-85056528073000449277700002https://www.aanda.org/articles/aa/abs/2018/11/aa33174-18/aa33174-18.html2018A&A...619A..39FFIS/05 - ASTRONOMIA E ASTROFISICA