
The UV condensers are simple chromatic objectives (made from fused silica) for the collection of light or for the imaging of light sources. A typical application e.g. would be to focus light from a sample to a spectrograph slit. For this purpose they feature an intermediate imaging quality and are optimized for high aperture angles.
This condenser is designed for a magnification
ratio M = β' = -5 (magnification 5) and is made from synthetic fused
silica. It can however also be used for collimation or other, similar magnification
ratios. The magnification ratio β' = -5 is achieved with about 533
mm distance between object and image. For different wavelengths the chromatism
makes necessary a refocusing which can be done by just moving the objective
(without need to alter the distance object to image).
The focal length is 70 mm at about 248 nm. At
this wavelength the wavefront error is about 3 Lambda, the spot diameter
is about 40 µm (measured in the enlarged image) with optimal focusing for
90 % objective diameter resp. about 100 µm with optimal focusing
for full diameter (full diameter of the Airy disc about 5.6 µm, for
comparison).
We have available for this condensors a drawing
of the holder dimensions with some additional data about integration and
a table about refocusing.
→ OUK 70.54
This condenser is designed for collimation (infinite
magnification) and is made from synthetic fused silica. It can however
also be used for finite magnification ratios. It is not color corrected.
The focal length f = 60 mm is a nominal value, at 248 nm the focal length is about 51 mm. At this wavelength the
wavefront error is about 10 to 20 Lambda, the spot diameter is about 20
µm (measured in the object) with optimal focusing for 90 % objective
diameter resp. about 40 µm with optimal focusing for full diameter
(full diameter of the Airy disc about 0.7 µm, for comparison).
We have available for this condensors a drawing
of the holder dimensions with some additional data about integration. → OUK 60.50