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In this example the lensing mass is assumed to lie at a redshift of 0.313, while the source lies at a redshift of 0.626. The lensing mass is assumed to be elliptical, and is several arc seconds in extent. The images produced by the lens are seen to cover a region of the sky approximately 20 arc seconds around the position of the lensing mass. A large variety of lensing effects is observed, including an Einstein cross when the lens and source are almost exactly aligned.