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

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1.2 Gravitational Lens<strong>in</strong>g<br />

Figure 1.2 – Illustration <strong>of</strong> the effects <strong>of</strong> convergence <strong>and</strong> shear on a circular source.<br />

Convergence magnifies the image isotropically, <strong>and</strong> shear deforms it to an ellipse.<br />

The magnification is then,<br />

µ = 1<br />

det A = 1<br />

(1 − κ) 2 − |γ| 2 . (1.31)<br />

Po<strong>in</strong>ts <strong>in</strong> the lens plane where the determ<strong>in</strong>ant equals zero, i.e. locations<br />

<strong>of</strong> <strong>in</strong>f<strong>in</strong>ite magnification, form closed curves, which are called critical curves.<br />

Their equivalent curves <strong>in</strong> the source plane are called caustics. Images along<br />

these curves will be magnified <strong>and</strong> distorted substantially.<br />

Strong lens<strong>in</strong>g occurs when the gravitational potential is extremely large,<br />

called a supercritical lens, where Σ ≥ Σ cr , <strong>and</strong> the shear <strong>and</strong> convergence are<br />

strong enough [see][](Hattori et al. 1999), <strong>of</strong>ten lead<strong>in</strong>g to multiple images <strong>of</strong><br />

a suitably positioned source. The effect causes great amplification <strong>and</strong> shear,<br />

<strong>of</strong>ten visible <strong>in</strong> centers <strong>of</strong> massive clusters as large distorted arcs ly<strong>in</strong>g near<br />

the critical curves. These have been observed with high quality <strong>and</strong> great<br />

detail with the Advanced Camera for Surveys (ACS) aboard the Hubble Space<br />

Telescope (HST ). Some examples <strong>of</strong> giant arcs can be seen <strong>in</strong> the clusters<br />

Abell 370 <strong>and</strong> Abell 2218 (see Figure 1.3).<br />

17

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