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                                              37.0°
                                                22.0°









                                                    (b)



                     (a)

        FIGURE 4.1  Immersion (a) and ATR (b) confi gurations for infrared
        microspectroscopy.

        used by optical microscopists to improve the spatial resolution of the
        method. Instead of liquid immersion oils, however, the infrared vari-
        ant employs ZnSe or Ge hemispheres as the immersion medium
        (see Fig. 4.1). In these attempts, the sample is interleaved between
        two hemispheres for transmission measurements or placed at the
        plano surface of a single hemisphere for attenuated total internal reflec-
        tion (ATR) measurements. Although immersion transmission infrared
        methods have been reported, sample thickness requirements and diffi-
        culty with coupling light through the sample do not make the method
        optimal for thin tissue  sections.  A method which is inherently an
        immersion method and solves the requirement for specially prepared
        samples is ATR imaging, which is the topic of this chapter. Finally,
        although this chapter focuses on infrared microspectroscopy, parallel
        developments in visible and fluorescence microscopy using solid
        immersion lenses took place at or about the same time. When possible,
        references will be given to highlight these developments.


   4.2 Theoretical Considerations
        The spatial characteristics of a focused beam of light can be estimated
        from diffraction theory. Equation (4.1) gives the diffraction limited
        diameter (x, y) for light focused to a point with a lens or objective
                                   122 λ
                                    .
                               d =                            (4.1)
                                  n sinθ
                                   1
        where λ= wavelength of light
              θ= half angle acceptance of the optic
             n =  refractive index of the medium in which the sample is
              1
                 immersed
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