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Figures (5)

Fig. 1
Fig. 1

A thin lens used at a magnification m.

Fig. 2
Fig. 2

The change in aperture on turning an unsymmetrical lens end-for-end.

Fig. 3
Fig. 3

A 1:1 printer with field flatteners.

Fig. 4
Fig. 4

An afocal 1:1 printer.

Fig. 5
Fig. 5

A long lens with a small rear window.

Equations (1)

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E = π k B sin 2 U ,