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dc.contributor.authorZolotov, Adi
dc.contributor.authorDekel, Avishai
dc.contributor.authorMandelker, Nir
dc.contributor.authorTweed, Dylan
dc.contributor.authorInoue, Shigeki
dc.contributor.authorDeGraf, Colin
dc.contributor.authorCeverino Rodríguez, Daniel 
dc.contributor.authorPrimack, Joel R.
dc.contributor.authorBarro, Guillermo
dc.contributor.authorFaber, Sandra M.
dc.contributor.otherUAM. Departamento de Física Teóricaes_ES
dc.date.accessioned2018-07-27T16:26:45Z
dc.date.available2018-07-27T16:26:45Z
dc.date.issued2015-07-01
dc.identifier.citationMonthly Notices of the Royal Astronomical Society 450.3 (2015): 2327-2353es_ES
dc.identifier.issn0035-8711 (print)es_ES
dc.identifier.issn1365-2966 (online)es_ES
dc.identifier.urihttp://hdl.handle.net/10486/684489
dc.descriptionThis article has been accepted for publication in Monthly Notices of the Royal Astronomical Society ©: 2015 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserveden_US
dc.description.abstractWe use cosmological simulations to study a characteristic evolution pattern of high redshift galaxies. Early, stream-fed, highly perturbed, gas-rich discs undergo phases of dissipative contraction into compact, star-forming systems (“blue” nuggets) at z∼4−2. The peak of gas compaction marks the onset of central gas depletion and inside-out quenching into compact ellipticals (red nuggets) by z ∼ 2. These are sometimes surrounded by gas rings or grow extended. We use cosmological simulations to study a characteristic evolution pattern of high redshift galaxies. Early, stream-fed, highly perturbed, gas-rich discs undergo phases of dissipative contraction into compact, star-forming systems (“blue” nuggets) at z∼4−2. The peak of gas compaction marks the onset of central gas depletion and inside-out quenching into compact ellipticals (red nuggets) by z ∼ 2. These are sometimes surrounded by gas rings or grow extended dry stellar envelopes. The compaction occurs at a roughly constant specific starformation rate (SFR), and the quenching occurs at a constant stellar surface density within the inner kpc ( 1). Massive galaxies quench earlier, faster, and at a higher 1 than lower-mass galaxies, which compactify and attempt to quench more than once. This evolution pattern is consistent with the way galaxies populate the SFR-radius-mass space, and with gradients and scatter across the main sequence. The compaction is triggered by an intense inflow episode, involving mergers, counter-rotating streams or recycled gas, and is commonly associated with violent disc instability. The contraction is dissipative, with the inflow rate >SFR, and the maximum 1 anti-correlated with the initial spin parameter, as predicted by Dekel & Burkert (2014). The central quenching is triggered by the high SFR and stellar/supernova feedback (possibly also AGN feedback) due to the high central gas density, while the central inflow weakens as the disc vanishes. Suppression of fresh gas supply by a hot halo allows the longterm maintenance of quenching once above a threshold halo mass, inducing the quenching downsizing dry stellar envelopes. The compaction occurs at a roughly constant specific starformation rate (SFR), and the quenching occurs at a constant stellar surface density within the inner kpc ( 1). Massive galaxies quench earlier, faster, and at a higher 1 than lower-mass galaxies, which compactify and attempt to quench more than once. This evolution pattern is consistent with the way galaxies populate the SFR-radius-mass space, and with gradients and scatter across the main sequence. The compaction is triggered by an intense inflow episode, involving mergers, counter-rotating streams or recycled gas, and is commonly associated with violent disc instability. The contraction is dissipative, with the inflow rate >SFR, and the maximum 1 anti-correlated with the initial spin parameter, as predicted by Dekel & Burkert (2014). The central quenching is triggered by the high SFR and stellar/supernova feedback (possibly also AGN feedback) due to the high central gas density, while the central inflow weakens as the disc vanishes. Suppression of fresh gas supply by a hot halo allows the longterm maintenance of quenching once above a threshold halo mass, inducing the quenching downsizingen_US
dc.description.sponsorshipThis work was supported by ISF grant 24/12, by GIF grant G-1052-104.7/2009, by a DIP grant, by the I-CORE Program of the PBC, by ISF grant 1829/12, and by NSF grants AST-1010033 and AST-1405962. SI and CD acknowledge Lady Davis Fellowships at HU. DC acknowledges support from MINECO grant AYA2012-31101, MICINN grant AYA-2009-13875-C03-02, and a Juan de la Cierva fellowshipen
dc.format.extent27 pag.es_ES
dc.format.mimetypeapplication/pdfen
dc.language.isoengen
dc.publisherOxford University Press on behalf of the Royal Astronomical Societyen_US
dc.relation.ispartofMonthly Notices of the Royal Astronomical Societyen_US
dc.rights© 2015 The Authorses_ES
dc.subject.otherGalaxies: elliptical and lenticular, cDen_US
dc.subject.otherGalaxies: evolutionen_US
dc.subject.otherGalaxies: formationen_US
dc.subject.otherGalaxies: kinematics and dynamicsen_US
dc.subject.otherGalaxies: spiralen_US
dc.titleCompaction and quenching of high-z galaxies in cosmological simulations: Blue and red nuggetsen_US
dc.typearticleen
dc.subject.ecienciaFísicaes_ES
dc.relation.publisherversionhttp://dx.doi.org/10.1093/mnras/stv740es_ES
dc.identifier.doi10.1093/mnras/stv740es_ES
dc.identifier.publicationfirstpage2327es_ES
dc.identifier.publicationissue3es_ES
dc.identifier.publicationlastpage2353es_ES
dc.identifier.publicationvolume450es_ES
dc.relation.projectIDGobierno de España. AYA2012-31101es_ES
dc.relation.projectIDGobierno de España. AYA-2009-13875- C03-02es_ES
dc.type.versioninfo:eu-repo/semantics/submittedVersionen
dc.rights.accessRightsopenAccessen
dc.facultadUAMFacultad de Ciencias


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