Compaction and quenching of high-z galaxies in cosmological simulations: Blue and red nuggets
Entity
UAM. Departamento de Física TeóricaPublisher
Oxford University Press on behalf of the Royal Astronomical SocietyDate
2015-07-01Citation
10.1093/mnras/stv740
Monthly Notices of the Royal Astronomical Society 450.3 (2015): 2327-2353
ISSN
0035-8711 (print); 1365-2966 (online)DOI
10.1093/mnras/stv740Funded by
This 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 fellowshipProject
Gobierno de España. AYA2012-31101; Gobierno de España. AYA-2009-13875- C03-02Editor's Version
http://dx.doi.org/10.1093/mnras/stv740Subjects
Galaxies: elliptical and lenticular, cD; Galaxies: evolution; Galaxies: formation; Galaxies: kinematics and dynamics; Galaxies: spiral; FísicaNote
This 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 reservedRights
© 2015 The AuthorsAbstract
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. 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 downsizing
Files in this item
Google Scholar:Zolotov, Adi
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Dekel, Avishai
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Mandelker, Nir
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Tweed, Dylan
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Inoue, Shigeki
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DeGraf, Colin
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Ceverino, Daniel
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Primack, Joel R.
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Barro, Guillermo
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Faber, Sandra M.
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