Thin disc, thick disc and halo in a simulated galaxy

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dc.creator Gibson, Brad K.
dc.creator Brook, C. B.
dc.creator Stinson, G. S.
dc.creator Kawata, D.
dc.creator House, E. L.
dc.creator Miranda, M. S.
dc.creator Maccio, A. V.
dc.creator Pilkington, K.
dc.creator Roskar, R.
dc.creator Wadsley, J.
dc.date.accessioned 2014-09-25T15:25:15Z
dc.date.available 2014-09-25T15:25:15Z
dc.date.issued 2012-10
dc.identifier.issn 1365-2966
dc.identifier.uri http://library2.smu.ca/xmlui/handle/01/25874
dc.description Publisher's version/PDF en_CA
dc.description.abstract Within a cosmological hydrodynamical simulation, we form a disc galaxy with subcomponents which can be assigned to a thin stellar disc, thick disc and a low-mass stellar halo via a chemical decomposition. The thin- and thick-disc populations so selected are distinct in their ages, kinematics and metallicities. Thin-disc stars are young (<6.6 Gyr), possess low velocity dispersion ([sigma]U,V,W =41, 31, 25 km s[superscript −1]), high [Fe/H] and low [O/Fe]. Conversely, the thick-disc stars are old (6.6 < age < 9.8Gyr), lag the thin disc by ∼21 km s[superscript −1], possess higher velocity dispersion ([sigma]U,V,W = 49, 44, 35 km s[superscript −1]) and have relatively low [Fe/H] and high [O/Fe]. The halo component comprises less than 4 per cent of stars in the ‘solar annulus’ of the simulation, has low metallicity, a velocity ellipsoid defined by [sigma]U,V,W = 62, 46, 45 km s[superscript −1] and is formed primarily in situ during an early merger epoch. Gas-rich mergers during this epoch play a major role in fuelling the formation of the old-disc stars (the thick disc). We demonstrate that this is consistent with studies which show that cold accretion is the main source of a disc galaxy’s baryons. Our simulation initially forms a relatively short (scalelength ∼1.7 kpc at z = 1) and kinematically hot disc, primarily from gas accreted during the galaxy’s merger epoch. Far from being a competing formation scenario, we show that migration is crucial for reconciling the short, hot, discs which form at high redshift in cold dark matter, with the properties of the thick disc at z = 0. The thick disc, as defined by its abundances, maintains its relatively short scalelength at z = 0 (2.31 kpc) compared with the total disc scalelength of 2.73 kpc. The inside-out nature of disc growth is imprinted in the evolution of abundances such that the metal-poor [alpha]-young population has a larger scalelength (4.07 kpc) than the more chemically evolved metal-rich [alpha]-young population (2.74 kpc). en_CA
dc.description.provenance Submitted by Janine Mills (janine.mills@smu.ca) on 2014-09-25T15:25:15Z No. of bitstreams: 1 gibson_b_k_article_2012_b.pdf: 895633 bytes, checksum: f57fe57abea11e62ba51b97271c99178 (MD5) en
dc.description.provenance Made available in DSpace on 2014-09-25T15:25:15Z (GMT). No. of bitstreams: 1 gibson_b_k_article_2012_b.pdf: 895633 bytes, checksum: f57fe57abea11e62ba51b97271c99178 (MD5) Previous issue date: 2012 en
dc.language.iso en en_CA
dc.publisher Royal Astronomical Society en_CA
dc.relation.uri http://dx.doi.org/10.1111/j.1365-2966.2012.21738.x
dc.subject.lcsh Disks (Astrophysics)
dc.subject.lcsh Hydrodynamics
dc.subject.lcsh Computer simulation
dc.subject.lcsh Galaxies -- Evolution
dc.subject.lcsh Galaxies -- Formation
dc.title Thin disc, thick disc and halo in a simulated galaxy en_CA
dc.type Text en_CA
dcterms.bibliographicCitation Monthly Notices of the Royal Astronomical Society 426(1), 690-700. (2012) en_CA
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Published Version: http://dx.doi.org/10.1111/j.1365-2966.2012.21738.x
 
 

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