In the drawings:
The light coming from the sample 7 travels in a detection beam path 9 in the cut out center of the annular lenses 1 to 4 and reaches a detection device, not shown.
Lenses 1 to 4 have the radii r, thicknesses d, distances a in mm, refractive indexes ne at wavelength 546 nm, Abbe numbers ve, and free diameters Frd indicated in the following table. Contrary to the positive distances between the lenses which are otherwise only possible and conventional, negative distances or the distance 0 mm are also possible. This is easy to understand: if the drilled lens were filled to form a normal lens, the lenses would penetrate one another because of the very presence of this negative distance of the lens vertexes.
NK5 and NFK5 are possible types of glass that may be used. The carrier glass 6 is planar and has a thickness of 0.17 mm.
Standard immersion oil with a refractive index ne=1.518 and a dispersion ve=47.37 is advantageously used as immersion liquid 8.
The angle β is varied by changing the distance from the focus point to the optical axis. For example, when the distance between the focus point and the optical axis is 12.5 mm, angle β is 82.5°; when this distance is 12.17 mm, angle β is 74.1°, etc.
Fields with a diameter of about 580 μm can be observed on the sample with this construction of the illumination optics according to the invention. This results in a significant advantage over the prior art because previously only fields of about 110 μm diameter could be observed.
This advantage is achieved substantially because separate illumination optics are used which can have a different focal length than the detection optics.
Another advantage is the possibility of reducing the penetration depth because angles β up to 81.2° can be realized with the illumination optics according to the invention, which corresponds to a numerical aperture of 1.50 when the refractive index of the immersion oil is 1.518. Because of the available long focal length by which the light source is imaged in the sample, it possible to vary the illumination angle or angle β substantially more accurately than in the prior art in which the illumination of the sample is carried out through a microscope objective.
Another substantial advantage consists in that the autofluorescence of the material from which the optical elements of the microscope objective are made in the prior art need not be taken into account because these elements are no longer penetrated by the illumination light (which corresponds to the excitation light in fluorescence microscopy).
Therefore, the entire optical system of these illumination optics can be optimized specifically to the shorter wavelengths of fluorescence excitation radiation, and it is now only necessary to correct the outside pupil area for a light bundle with a small diameter so that the optical system can be designed in an uncomplicated manner.
While the foregoing description and drawings represent the present invention, it will be obvious to those skilled in the art that various changes may be made therein without departing from the true spirit and scope of the present invention.
Number | Date | Country | Kind |
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10 2006 039 976.5 | Aug 2006 | DE | national |