Editing Microscopy (section)

==== Differential interference contrast ====
{{Main|Differential interference contrast microscopy}}
Superior and much more expensive is the use of '''interference contrast'''. Differences in optical density will show up as differences in relief. A nucleus within a cell will actually show up as a globule in the most often used '''differential interference contrast''' system according to [[Georges Nomarski]]. However, it has to be kept in mind that this is an ''optical effect'', and the relief does not necessarily resemble the true shape. Contrast is very good and the condenser aperture can be used fully open, thereby reducing the depth of field and maximizing resolution.

The system consists of a special prism ([[Nomarski prism]], [[Wollaston prism]]) in the condenser that splits light in an ordinary and an extraordinary beam. The spatial difference between the two beams is minimal (less than the maximum resolution of the objective). After passage through the specimen, the beams are reunited by a similar prism in the objective.

In a homogeneous specimen, there is no difference between the two beams, and no contrast is being generated. However, near a refractive boundary (say a nucleus within the cytoplasm), the difference between the ordinary and the extraordinary beam will generate a relief in the image. Differential interference contrast requires a [[polarized light]] source to function; two polarizing filters have to be fitted in the light path, one below the condenser (the polarizer), and the other above the objective (the analyzer).

Note: In cases where the optical design of a microscope produces an appreciable lateral separation of the two beams we have the case of [[classical interference microscopy]], which does not result in relief images, but can nevertheless be used for the quantitative determination of mass-thicknesses of microscopic objects.