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dc.contributor.authorKrieger, Nico
dc.contributor.authorBolatto, Alberto D.
dc.contributor.authorWalter, Fabian
dc.contributor.authorLeroy, Adam K.
dc.contributor.authorZschaechner, Laura K.
dc.contributor.authorMeier, David S.
dc.contributor.authorOtt, Jürgen
dc.contributor.authorWeiss, Axel
dc.contributor.authorMills, Elisabeth
dc.contributor.authorLevy, Rebecca C.
dc.contributor.authorVeilleux, Sylvain
dc.contributor.authorGorski, Mark
dc.date.accessioned2021-01-04T20:22:51Z
dc.date.available2021-01-04T20:22:51Z
dc.date.issued2019-08-12
dc.identifier.citationNico Krieger et al 2019 ApJ 881 43en_US
dc.identifier.urihttp://hdl.handle.net/1808/31024
dc.description.abstractWe present 0farcs15 (~2.5 pc) resolution ALMA CO(3–2) observations of the starbursting center in NGC 253. Together with archival ALMA CO(1–0) and CO(2–1) data, we decompose the emission into disk and nondisk components. We find ~7%–16% of the CO luminosity to be associated with the nondisk component (1.2–4.2 × 107 K km s−1 pc2). The total molecular gas mass in the center of NGC 253 is ~3.6 × 108 M ⊙ with ~0.5 × 108 M ⊙ (~15%) in the nondisk component. These measurements are consistent across independent mass estimates through three CO transitions. The high-resolution CO(3–2) observations allow us to identify the molecular outflow within the nondisk gas. Using a starburst conversion factor, we estimate the deprojected molecular mass outflow rate, kinetic energy, and momentum in the starburst of NGC 253. The deprojected molecular mass outflow rate is in the range of ~14–39 M ⊙ yr−1 with an uncertainty of 0.4 dex. The large spread arises due to different interpretations of the kinematics of the observed gas while the errors are due to unknown geometry. The majority of this outflow rate is contributed by distinct outflows perpendicular to the disk, with a significant contribution by diffuse molecular gas. This results in a mass-loading factor $\eta ={\dot{M}}_{\mathrm{out}}/{\dot{M}}_{\mathrm{SFR}}$ in the range η ~ 8−20 for gas ejected out to ~300 pc. We find the kinetic energy of the outflow to be ~2.5–4.5 × 1054 erg and a typical error of ~0.8 dex, which is ~0.1% of the total or ~8% of the kinetic energy supplied by the starburst. The outflow momentum is 4.8–8.7 × 108 M ⊙ km s−1 (~0.5 dex error) or ~2.5%–4% of the kinetic momentum released into the ISM by the feedback. The unknown outflow geometry and launching sites are the primary sources of uncertainty in this study.en_US
dc.publisherAmerican Astronomical Societyen_US
dc.rights© 2019. The American Astronomical Society. All rights reserved.en_US
dc.subjectGalaxies: individual (NGC 253)en_US
dc.subjectGalaxies: ISMen_US
dc.subjectGalaxies: starbursten_US
dc.subjectISM: jets and outflowsen_US
dc.subjectISM: kinematics and dynamicsen_US
dc.titleThe Molecular Outflow in NGC 253 at a Resolution of Two Parsecsen_US
dc.typeArticleen_US
kusw.kuauthorMills, Elisabeth
kusw.kudepartmentPhysics and Astronomyen_US
dc.identifier.doi10.3847/1538-4357/ab2d9cen_US
dc.identifier.orcidhttps://orcid.org/0000-0003-1104-2014en_US
dc.identifier.orcidhttps://orcid.org/0000-0002-5480-5686en_US
dc.identifier.orcidhttps://orcid.org/0000-0003-4793-7880en_US
dc.identifier.orcidhttps://orcid.org/0000-0002-2545-1700en_US
dc.identifier.orcidhttps://orcid.org/0000-0002-9919-8672en_US
dc.identifier.orcidhttps://orcid.org/0000-0001-9436-9471en_US
dc.identifier.orcidhttps://orcid.org/0000-0001-8224-1956en_US
dc.identifier.orcidhttps://orcid.org/0000-0003-4678-3939en_US
dc.identifier.orcidhttps://orcid.org/0000-0001-8782-1992en_US
dc.identifier.orcidhttps://orcid.org/0000-0003-2508-2586en_US
dc.identifier.orcidhttps://orcid.org/0000-0002-3158-6820en_US
kusw.oaversionScholarly/refereed, publisher versionen_US
kusw.oapolicyThis item meets KU Open Access policy criteria.en_US
dc.rights.accessrightsopenAccessen_US


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