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Chapter Fourteen
Figure 14.20
APetzval modification using dense barium crowns, with the split rear
doublet widely spaced so that its flint element acts as a field flattener.
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Some Forty-Four Lens Designs
Figure 14.21
Amodification of Fig. 14.20 which splits the positive elements to allow
both improved performance and a significant increase of the speed to f/1.4.
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Chapter Fourteen
Figure 14.22
Asplit front crown in this Petzval lens allows a speed of f/1.25 using ordi-
nary glasses. But notice the extremely short back focal length (which facilitates the good
performance by reducing the element powers compared with  those required when a
longer back focus is provided).
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Some Forty-Four Lens Designs
Figure  14.23
The  R-Biotar,  an  extremely  high-speed  lens  of  simple  construction,
designed as a radiographic camera lens, controls the higher-order aberrations by care-
ful spacing and power distribution.
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Chapter Fourteen
Figure 14.24
When the thickness is allowed to vary, the split-front triplet often takes
this form, where the first three elements look a bit like the front member of a double-
Gauss design.
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Some Forty-Four Lens Designs
Figure 14.25
Adirect descendant from the split-front triplet design, this design replaces
elements two and three with a triplet component using a low-index glass instead of air
to space elements two and three apart, plus a Tessar-type rear component.
Chapter Fourteen
Figure 14.26
Areally high-speed Sonnar.
Some Forty-Four Lens Designs
Figure 14.27
The meniscus inner crown of the split-front triplet can advantageously be
made a doublet. This is about the simplest of the many modifications that this powerful
basic design form has undergone.
Chapter Fourteen
Figure 14.28
An example of a high-power microscope objective in which the apla-
natic  front  hyperhemisphere  is  modified  by  introducing  a  concave front surface
which, being near the focus, acts as a field flattener. Note also the use of calcium flu-
oride and FK51 glass to correct the secondary spectrum.
Some Forty-Four Lens Designs
Figure 14.29
Three singlet correctors, of the same glass, whose power totals zero,
are used to correct the aberrations of the spherical-surfaced Cassegrain configura-
tion without introducing either primary or secondary chromatic aberration (but
not without spherochromatism).
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