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22<br />

14<br />

Point grid<br />

From the diffraction image of the<br />

point grid (Fig. 9), the 0th and the<br />

first secondary maxima in the horizontal<br />

axis are faded out via the slit.<br />

In the intermediate image, a line grid<br />

then appears in the perpendicular<br />

direction (Fig. 11), and at an angle of<br />

45° when the slit is oriented diagonally<br />

(Fig. 12). A particularly remarkable<br />

feature of the artificially produced<br />

45° grating is that the lines are<br />

closer to each other than in other images.<br />

This is bound to be the case because<br />

the secondary maxima in the<br />

45° diffraction image are further<br />

away from the 0th maximum than in<br />

the perpendicular or horizontal diffraction<br />

images.<br />

With these experiments, Abbe finally<br />

showed that the image in the<br />

microscope is created in the space<br />

between the primary diffraction image<br />

(back focal plane of the objective)<br />

and the intermediate image<br />

plane through interference of diffracted<br />

light waves.<br />

In a further experiment, Abbe<br />

demonstrated why the resolution<br />

formula is<br />

d=<br />

�<br />

2nx sin �<br />

numerical aperture.<br />

2 x n x sin � =<br />

Abbe pushed the point-shaped light<br />

source to the edge (known as<br />

oblique illumination): therefore, the<br />

1st secondary maximum can be twice<br />

as distant as in straight illumination,<br />

i. e. the distance d between two<br />

points or lines can be twice as small.<br />

On this basis, Abbe had already developed<br />

the illumination apparatus<br />

with focusing condenser in 1872 (Fig.<br />

14). In today’s microscopy, we use unilateral<br />

oblique illumination to achieve<br />

full resolution with the maximum<br />

condenser aperture.<br />

The theory of microscope image<br />

formation and its practical implementation<br />

defined the resolution limits<br />

and thus enabled the scientific construction<br />

of microscopes. Abbe could<br />

11 12<br />

then concentrate on the correction of<br />

spherical and chromatic aberration.<br />

He realized that this requires the<br />

development of special glass materials.<br />

His collaboration with the glass<br />

maker Otto Schott (1851-1935) started<br />

in 1879, and the first Apochromat<br />

objectives featuring high color fidelity<br />

were already launched in 1886.<br />

In 1893, August Köhler (1866-<br />

1948) developed his illumination<br />

technique with separate control of<br />

luminous-field diaphragm and condenser<br />

aperture on the basis of<br />

Abbe’s results. Köhler also developed<br />

the microscope with ultraviolet light,<br />

which was primarily built to increase<br />

the resolution by a factor of 2 relative<br />

to green light. Finally, the phase<br />

contrast technique from the Dutch<br />

physicist Frits Zernike also is attributable<br />

to manipulation in the back<br />

focal plane of the objective.<br />

With his theory and experiments,<br />

Ernst Abbe decisively shaped the development<br />

of microscopy in the 19th<br />

and 20th centuries. Numerous Nobel<br />

prizes are directly or indirectly con-<br />

Innovation 15, <strong>Carl</strong> <strong>Zeiss</strong> AG, 2005

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