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Risa Wechsler - Astronomy and Astrophysics

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M 200<br />

Lensing Mass<br />

r200 [h !1 Cluster Mpc] Size<br />

10 14<br />

10 13<br />

10 12<br />

2.0<br />

1.0<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

S<br />

M200 = A Ngal A= 2.1±0.4 ×10 11<br />

S= 1.56±0.07<br />

χ 2 = 11.1 DOF=10<br />

0.4<br />

6 8 10 20 40 60 80 100<br />

N gals<br />

lensing mass<br />

Sigma diff<br />

1000<br />

several ways to<br />

measure the<br />

scaling between<br />

cluster richness<br />

<strong>and</strong> “mass”<br />

Real Data<br />

• need to underst<strong>and</strong> velocity bias (as a function of radius & L)<br />

1<br />

Sheldon et al 2005 (in prep)<br />

• can measure scatter<br />

10 100<br />

cluster sizes<br />

100<br />

1 10<br />

McKay et al 2005 (in prep)<br />

100 1000<br />

Ngals Hansen et al 2005,<br />

ApJ in press<br />

Velocity Dispersion<br />

• well understood theoretically<br />

• selection biases <strong>and</strong> centering effects need to be understood<br />

• no direct method to measure scatter<br />

cluster velocity dispersions<br />

• need additional data (spectra), which is typically redshift dependent<br />

1000.0<br />

• depends on galaxy background, degenerate with cosmology<br />

cluster-cluster correlation function<br />

• no direct method to measure scatter<br />

ξ(r)<br />

Cluster Correlation<br />

Function<br />

100.0<br />

10.0<br />

• uncertainties in redshifts can bias measurements<br />

probably have more scatter than Lx, SZ,<br />

1.0<br />

but order of magnitude easier to find<br />

0.1<br />

1 10 100<br />

r [Mpc/h]

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