MAGICC haloes: confronting simulations with observations of the circumgalactic medium at z = 0

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dc.creator Stinson, G. S.
dc.creator Brook, C.
dc.creator Prochaska, J. Xavier
dc.creator Hennawi, Joe
dc.creator Shen, Sijing
dc.creator Wadsley, J.
dc.creator Pontzen, Andrew
dc.creator Couchman, H. M. P.
dc.creator Quinn, T.
dc.creator Maccio, Andrea V.
dc.creator Gibson, Brad K.
dc.date.accessioned 2018-04-18T15:16:23Z
dc.date.available 2018-04-18T15:16:23Z
dc.date.issued 2012-09
dc.identifier.issn 0035-8711
dc.identifier.uri http://library2.smu.ca/handle/01/27428
dc.description Publisher's Version/PDF
dc.description.abstract We explore the circumgalactic medium (CGM) of two simulated star-forming galaxies with luminosities L &asymp; 0.1 and 1 L<sup>★</sup> generated using the smooth particle hydrodynamic code GASOLINE. These simulations are part of the Making Galaxies In a Cosmological Context (MAGICC) program in which the stellar feedback is tuned to match the stellar mass&ndash;halo mass relationship. For comparison, each galaxy was also simulated using a &lsquo;lower feedback&rsquo; (LF) model which has strength comparable to other implementations in the literature. The &lsquo;MAGICC feedback&rsquo; (MF) model has a higher incidence of massive stars and an approximately two times higher energy input per supernova. Apart from the low-mass halo using LF, each galaxy exhibits a metal-enriched CGM that extends to approximately the virial radius. A significant fraction of this gas has been heated in supernova explosions in the disc and subsequently ejected into the CGM where it is predicted to give rise to substantial O VI absorption. The simulations do not yet address the question of what happens to the O VI when the galaxies stop forming stars. Our models also predict a reservoir of cool H I clouds that show strong Ly&alpha; absorption to several hundred kpc. Comparing these models to recent surveys with the Hubble Space Telescope, we find that only the MF models have sufficient O VI and H I gas in the CGM to reproduce the observed distributions. In separate analyses, these same MF models also show better agreement with other galaxy observables (e.g. rotation curves, surface brightness profiles and H I gas distribution). We infer that the CGM is the dominant reservoir of baryons for galaxy haloes. en_CA
dc.description.provenance Submitted by Betty McEachern (betty.mceachern@smu.ca) on 2018-04-18T15:16:23Z No. of bitstreams: 1 Gibson_Brad_K_article_2012_g.pdf: 2535666 bytes, checksum: 45d28ad9571a909d67db5d8e2defa2e4 (MD5) en
dc.description.provenance Made available in DSpace on 2018-04-18T15:16:23Z (GMT). No. of bitstreams: 1 Gibson_Brad_K_article_2012_g.pdf: 2535666 bytes, checksum: 45d28ad9571a909d67db5d8e2defa2e4 (MD5) Previous issue date: 2012-09 en
dc.language.iso en en_CA
dc.publisher Wiley-Blackwell en_CA
dc.relation.uri https://dx.doi.org/10.1111/j.1365-2966.2012.21522.x
dc.rights This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society ©: 2012 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.
dc.subject.lcsh Galaxies -- Evolution
dc.subject.lcsh Galactic halos
dc.subject.lcsh Hydrodynamics -- Simulation methods
dc.title MAGICC haloes: confronting simulations with observations of the circumgalactic medium at z = 0 en_CA
dc.type Text en_CA
dcterms.bibliographicCitation Monthly Notices of the Royal Astronomical Society 425(2), 1270-1277. (2012) en_CA
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This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society ©: 2012 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.
 
Published Version: https://dx.doi.org/10.1111/j.1365-2966.2012.21522.x
 
 

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