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dc.contributor.authorIbata, Rodrigo A.en_US
dc.contributor.authorLewis, Geraint F.en_US
dc.contributor.authorMcConnachie, Alan W.en_US
dc.contributor.authorMartin, Nicolas F.en_US
dc.contributor.authorIrwin, Michael J.en_US
dc.contributor.authorFerguson, Annette M. N.en_US
dc.contributor.authorBabul, Arifen_US
dc.contributor.authorBernard, Edouard J.en_US
dc.contributor.authorChapman, Scott C.en_US
dc.contributor.authorCollins, Michelleen_US
dc.contributor.authorFardal, Marken_US
dc.contributor.authorMackey, A. D.en_US
dc.contributor.authorNavarro, Julioen_US
dc.contributor.authorPenarrubia, Jorgeen_US
dc.contributor.authorRich, R. Michaelen_US
dc.contributor.authorTanvir, Nialen_US
dc.contributor.authorWidro, Lawrenceen_US
dc.date.accessioned2014-03-12T19:20:54Z
dc.date.available2014-03-12T19:20:54Z
dc.date.issued2013-11-22en_US
dc.identifier.citationIbata, Rodrigo A., Geraint F. Lewis, Alan W. McConnachie, Nicolas F. Martin, et al. 2013. "The large-scale structure of the halo of the Andromeda Galaxy Part I: global stellar density, morphology and metallicity properties." The Astrophysical Journal780(2):128en_US
dc.identifier.issn0004-637X
dc.identifier.urihttp://hdl.handle.net/10222/45344
dc.identifier.urihttp://dx.doi.org/10.1088/0004-637X/780/2/128
dc.description.abstractWe present an analysis of the large-scale structure of the halo of the Andromeda galaxy, based on the Pan-Andromeda Archeological Survey (PAndAS), currently the most complete map of resolved stellar populations in any galactic halo. Despite copious substructure, the global halo populations follow closely power law profiles that become steeper with increasing metallicity. We divide the sample into stream-like populations and a smooth halo component. Fitting a three-dimensional halo model reveals that the most metal-poor populations ([Fe/H]-0.6). The space density of the smooth metal-poor component has a global power-law slope of -3.08+/-0.07, and a non-parametric fit shows that the slope remains nearly constant from 30kpc to 300kpc. The total stellar mass in the halo at distances beyond 2 degrees is 1.1x10^10 Solar masses, while that of the smooth component is 3x10^9 Solar masses. Extrapolating into the inner galaxy, the total stellar mass of the smooth halo is plausibly 8x10^9 Solar masses. We detect a substantial metallicity gradient, which declines from [Fe/H]=-0.7 at R=30kpc to [Fe/H]=-1.5 at R=150kpc for the full sample, with the smooth halo being 0.2dex more metal poor than the full sample at each radius. While qualitatively in-line with expectations from cosmological simulations, these observations are of great importance as they provide a prototype template that such simulations must now be able to reproduce in quantitative detail.en_US
dc.relation.ispartofThe Astrophysical Journal
dc.titleThe large-scale structure of the halo of the Andromeda Galaxy Part I: global stellar density, morphology and metallicity propertiesen_US
dc.title.alternativearXiv:1311.5888 [astro-ph]en_US
dc.typearticleen_US
dc.identifier.volume780
dc.identifier.issue2
dc.identifier.startpage128en_US
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