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Evanescent W ave Imaging   113


        sample type is known as the reststrahlen effect, in which the sample
        becomes a perfect reflector near an absorption band. Last it should be
        remembered that the refractive index of a sample changes dramatically in
        and around an absorption. These effects manifest themselves in the spec-
        tra in a variety of ways and make the interpretation of the spectra and the
        identification of disease states very difficult. From a quantitative perspec-
        tive, the adherence of the Beer Lambert law dictates that the sole mecha-
        nism for the attenuation of light must be absorption and that the optical
        path length through the sample be well known.
            Starting out with the simple case of a blood vessel or vesicle within
        the tissue, the interface is comprised of air and tissue and the difference
        in refractive index between these two materials is ~0.40 units. When a
        spectrum is obtained on such an interface, portions of the light
        undergo specular reflection and dispersion which manifest them-
        selves in the spectrum as derivative shaped peaks Sommer and
        Katon illustrated these dispersive band shapes in infrared microspec-
                27
        troscopy.  Later, Stewart and Sommer demonstrated that these opti-
        cal nonlinearities increase with a greater difference in refractive
        indices between two materials and that the magnitude of the effect
        increases with a decreasing spatial domain of one material embedded



                                                Reference Spectrum







             % Transmission                        Δn  = 0.03
                                                     d




                                                   Δn  = 0.12
                                                     d



                                                       = 0.58
                                                   Δn d


             900    850    800    750    700     650    600
                                          –1
                              Wavenumber (cm )
        FIGURE 4.6  Band distortion due to refractive index differences. [J. M.
        Chalmers and P. R. Griffi ths (eds.), Handbook of Vibrational Spectroscopy,
        Vol. 2, page 1381, fi gure 14 (John Wiley & Sons, Inc., West Sussex, UK
        2002).] (Waiting on permission).
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