2012
DOI: 10.1111/j.1365-2966.2012.20980.x
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A simple parametric model for spherical galaxy clusters

Abstract: We present an analytic parametric model to describe the baryonic and dark matter distributions in clusters of galaxies with spherical symmetry. It is assumed that the dark matter density follows a Navarro, Frenk and White (NFW) profile and that the gas pressure is described by a generalised NFW (GNFW) profile. By further demanding hydrostatic equilibrium and that the gas fraction is small throughout the cluster, one obtains unique functional forms, dependent on basic cluster parameters, for the radial profiles… Show more

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Cited by 28 publications
(45 citation statements)
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“…It is at higher redshift, z = 0.412 (Böhringer et al 2000) so the large value for θ s of ≈4.5 arcmin preferred by Planck is slightly surprising. Figure 34 shows the posteriors on θ s and Y tot produced by AMI and Planck, as well as the region of the space predicted by the physical model described in Olamaie et al (2012) assuming the universal pressure profile for the gas, and the Tinker mass function (Tinker et al 2008). The AMI posterior is much more consistent with the prediction than the Planck posterior; also our simulations have shown that if the correct value were θ s ≈ 4.5, we should recover it even if the profile deviates from the universal profile.…”
Section: Rxc J22286+2036 (Psz1 G08330-3101)mentioning
confidence: 99%
See 1 more Smart Citation
“…It is at higher redshift, z = 0.412 (Böhringer et al 2000) so the large value for θ s of ≈4.5 arcmin preferred by Planck is slightly surprising. Figure 34 shows the posteriors on θ s and Y tot produced by AMI and Planck, as well as the region of the space predicted by the physical model described in Olamaie et al (2012) assuming the universal pressure profile for the gas, and the Tinker mass function (Tinker et al 2008). The AMI posterior is much more consistent with the prediction than the Planck posterior; also our simulations have shown that if the correct value were θ s ≈ 4.5, we should recover it even if the profile deviates from the universal profile.…”
Section: Rxc J22286+2036 (Psz1 G08330-3101)mentioning
confidence: 99%
“…Alternatively, r X and M X for some overdensity radius X can be recovered given a redshift, a concentration parameter c X ≡ r X /r s and some model or scaling relationship for translating Y into mass (e.g. Planck Collaboration XX 2014; Olamaie et al 2012). Physical modelling will not be addressed in this paper.…”
Section: Cluster Modelmentioning
confidence: 99%
“…For the cluster model, we used a Navarro-FrenkWhite (NFW; Navarro, Frenk & White 1997) dark matter profile in hydrostatic equilibrium with a gas pressure distribution described by a generalised NFW (GNFW; Nagai, Kravtsov & Vikhlinin 2007) profile with the shape parameters given in Arnaud et al (2010); for more details of the model see Olamaie, Hobson & Grainge (2012). We refer to this as the DM-GNFW model.…”
Section: Cluster Analysismentioning
confidence: 99%
“…We use the model described in Olamaie et al (2012) and (2013), with its corresponding assumptions on the dynamical state of the cluster (model I). As shown in Olamaie et al (2012) and(2013), the model leads to radial profiles for clusters physical properties that are consistent both with numerical simulations and multi wavelength observations of clusters (see e.g.…”
Section: Modelling the X-ray Surface Brightnessmentioning
confidence: 99%
“…Sarazin 1988;Vikhlinin et al 2005Vikhlinin et al , 2006LaRoque et al 2006; AMI Consortium: Olamaie et al 2012 andPlanck Collaboration et al 2013). These radial profiles (e.g.…”
Section: Introductionmentioning
confidence: 99%