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In the previous section we assumed that both lens and source where just
point masses. When the lens is extended, you can get multiple images
(3,5,7,...), depending on the impact parameter and the mass
distribution of the lens. If the source is extended as well, then
different parts of the source may be deflected and amplified in various
ways, and so the image may be highly deformed. We are now in a position
to look for applications. To wet your appetite, let me show you two
beautiful examples.
Figure 12.3 shows an Einstein ring. The lens is
probably an elliptical galaxy, and the source a more distant
spiral. Because of the near perfect alignment, the spiral has been
imaged into a ring.
Figure 12.4 shows how a nearby spiral galaxy has
lensed a very distant background quasar and produced multiple images of
it, in this case five.
Figure 12.3:
Hubble Space Telescope image of an Einstein ring, where a
fortuitous alignment has caused an intervening elliptical galaxy (the
central spot) to lens a background spiral galaxy into a ring.
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Figure 12.4:
Hubble Space Telescope image of the `Einstein cross',
where a distant quasar has been lensed into multiple images by an
intervening spiral galaxy.
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Next: Micro-lensing
Up: The lens equation
Previous: Point-like lens and source
Tom Theuns
平成19年2月7日