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MODULATION CONTRAST MICROSCOPY         169

                       which uses a related optical system. Like DIC optics, MCM systems produce images
                       that have a three-dimensional or shadow-cast quality, making objects appear as though
                       they were illuminated by a low-angle light source (Fig. 10-10). In both MCM and DIC,
                       brightly illuminated and shadowed edges correspond to optical path gradients (phase
                       gradients) of opposite slope in the specimen, but unlike DIC, the MCM system does not
                       require crystalline DIC prisms. Although resolution and detection sensitivity of the
                       Hoffman MCM system are somewhat reduced compared with DIC, the MCM produces
                       superior images at lower magnifications, allows optical sectioning of rounded cell spec-
                       imens, and offers certain advantages over DIC optics, including the ability to examine
                       cells on birefringent plastic substrates such as cell culture dishes. The Hoffman modu-
                       lation contrast system is commercially available through Modulation Optics, Inc.,
                       Greenvale, New York.


                       Contrast Methods Using Oblique Illumination

                       Those who test optical surfaces will already be familiar with the essentials of the
                       schlieren system, which is related to the well-known knife edge test first employed by
                       Leon Foucault in 1859 for measuring the radius of curvature of a lens surface. Toepler
                       later used the method to examine variations in the refractive index of a transparent
                       medium in a sample cell, where inhomogeneities in the medium appear as high contrast


































                       Figure 10-10
                       Mouse blastocysts, modulation contrast microscopy. As in DIC microscopy, variations in
                       intensity of the image correspond to gradients in optical path length in the specimen. The
                       contrast image is generated by blocking one sideband of the diffracted light. There is no
                       dependence on polarized light and no dual-beam interference mechanism as in DIC
                       microscopy. (Image courtesy of Mahmud Saddiqi, Johns Hopkins University.)
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