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Mass and Light distributions in Clusters of Galaxies - Henry A ...

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3.11 Discussion <strong>and</strong> conclusions<br />

Table 3.3 – Parameters <strong>of</strong> Schechter fits to the Lum<strong>in</strong>osity function<br />

Cluster radial range α M ∗<br />

(h −1 Mpc)<br />

A1703 0 − 0.3 −0.95 ± 0.05 −21.4 ± 0.6<br />

0.3 − 0.8 −1.08 ± 0.08 −21.7 ± 0.8<br />

0.8 − 2.5 −1.24 ± 0.2 −21.8 ± 3<br />

A370 0 − 0.3 −1 ± 0.04 −22.4 ± 0.6<br />

0.3 − 1 −1.12 ± 0.05 −22.1 ± 0.7<br />

1 − 2.2 −1.18 ± 0.09 −22.8 ± 1<br />

RXJ1347-11 0 − 0.8 −1 ± 0.06 −21.6 ± 0.5<br />

0.8 − 2 −1.12 ± 0.1 −22 ± 2<br />

3.11 Discussion <strong>and</strong> conclusions<br />

In this paper we have compared <strong>in</strong> detail the dark <strong>and</strong> lum<strong>in</strong>ous properties <strong>of</strong><br />

three high mass galaxy clusters, A1703, A370 <strong>and</strong> RXJ1347-11, <strong>and</strong> exam<strong>in</strong>ed<br />

the relation between mass <strong>and</strong> light all the way out to the virial radius.<br />

We have further applied the WL dilution approach previously developed for<br />

A1689 (Medez<strong>in</strong>ski et al. 2007) as an alternative means <strong>of</strong> obta<strong>in</strong><strong>in</strong>g the<br />

LF <strong>and</strong> light pr<strong>of</strong>iles <strong>of</strong> galaxy clusters. This is based on the dilution <strong>of</strong> the<br />

lens<strong>in</strong>g distortion signal by unlensed cluster members, <strong>and</strong> has the advantage<br />

<strong>of</strong> be<strong>in</strong>g <strong>in</strong>dependent <strong>of</strong> density fluctuations <strong>in</strong> the background.<br />

We have exam<strong>in</strong>ed clusters A1703, A370 <strong>and</strong> RXJ1347-11 for which data<br />

<strong>of</strong> exceptional quality has been taken with Subaru/Suprime-Cam <strong>in</strong> multiple<br />

passb<strong>and</strong>s. We have shown how a careful separation <strong>of</strong> the cluster,<br />

foreground, <strong>and</strong> background galaxies can be achieved us<strong>in</strong>g weak lens<strong>in</strong>g <strong>in</strong>formation<br />

<strong>and</strong> galaxy colors. We also make use <strong>of</strong> the cluster<strong>in</strong>g <strong>of</strong> cluster<br />

members, f<strong>in</strong>d<strong>in</strong>g the cluster members are conf<strong>in</strong>ed to a dist<strong>in</strong>ct region <strong>of</strong><br />

CC space with relatively small mean radial distances. We have constructed<br />

a reliable background sample for WL measurements, by select<strong>in</strong>g red background<br />

galaxies whose WL signal rises all the way to the center <strong>of</strong> the cluster,<br />

<strong>and</strong> add<strong>in</strong>g to those the fa<strong>in</strong>t cloud <strong>of</strong> very blue galaxies, whose WL signal<br />

we have shown is <strong>in</strong> good agreement with the red galaxies. We have avoided<br />

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