2014
DOI: 10.1051/0004-6361/201220956
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On the relation between metallicity and RGB color in HST/ACS data

Abstract: Context. The determination of stellar metallicity and its gradient in external galaxies is a difficult task, but crucial for the understanding of galaxy formation and evolution. Aims. The color of the Red Giant Branch (RGB) can be used to determine metallicities of stellar populations that have only shallow photometry. We will quantify the relation between metallicity and color in the widely used HST/ACS filters F606W and F814W. Methods. We use a sample of globular clusters from the ACS Globular Cluster Survey… Show more

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Cited by 20 publications
(28 citation statements)
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“…However the metallicities obtained from RGB colours have large uncertainties. Streich et al (2014) estimate a lower uncertainty of 0.3 dex for metallicities derived for colours F 606W − F 814W < 1.2 whereas metallicities derived for colours redder than 1. …”
Section: Discussionmentioning
confidence: 67%
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“…However the metallicities obtained from RGB colours have large uncertainties. Streich et al (2014) estimate a lower uncertainty of 0.3 dex for metallicities derived for colours F 606W − F 814W < 1.2 whereas metallicities derived for colours redder than 1. …”
Section: Discussionmentioning
confidence: 67%
“…However, because the colours of the RGB stars are more sensitive to metallicity than to age and because there is a direct relation between RGB colours and metallicities (see e.g. Streich et al 2014, and references therein), one can assume that the colour profiles presented in the previous section reflect metallicity profiles. This assumption will allow us to compare our results with other work in which metallicities of individual fields and/or metallicity profiles of stellar haloes are constructed.…”
Section: Discussionmentioning
confidence: 99%
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“…While both haloes are richly substructured and qualitatively agree with the ΛCDM paradigm of galaxy formation, they display significant differences. The Milky Way halo has a weak to no metallicity gradient (Sesar et al 2011;Xue et al 2015) and its stellar density distribution can be described by a broken power-law -within 25 − 30 kpc, it follows an oblate, ρ ∝ r −γ powerlaw distribution with index γ ∼ 2.5 − 3 (Yanny et al 2000;Bell et al 2008;Jurić et al 2008;van Vledder et al 2016) whereas a more rapidly declining stellar density is detected beyond ∼ 30 kpc, with γ ∼ 3.5 (Deason et al 2011;Sesar et al 2011;Deason et al 2014;Cohen et al 2015;Slater et al 2016). M31, on the other hand, has a clear metallicity gradient with a 1 dex variation in [Fe/H] from 10 to ∼100 kpc (Gilbert et al 2014;Ibata et al 2014) and its stellar density distribution can be described by a single power-law with γ ∼ 3.3 (Guhathakurta et al 2005;Gilbert et al 2012).…”
Section: Introductionmentioning
confidence: 99%