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104    Cha pte r  F o u r



























                                                       (b)


                 (a)
        FIGURE 4.2 Adapted from Nakano and Kawata and Esaki et al. Confi guration
        employed by Nakano and Kawata (b) and that by Esaki et al. (a). [L. L. Lewis
        and A. J. Sommer, Applied Spectroscopy, Vol. 54, No. 2, page 325, fi gure 1
        (Society for Applied Spectroscopy, Frederick, Md., 2000).]



        was not employed, no improvement in spatial resolution was realized.
        Tajima, of the Shimadzu Corporation, demonstrated ATR mapping
                                   24
        with an automated microscope.  In this case, the sample was raised
        into the hemisphere for sample analysis then lowered to access sub-
        sequent sampling points. While this method was acceptable for hard
        stable surfaces, another method was needed to study soft surfaces due
        to the fact that some material from one sample point could transfer to
        the hemisphere and contaminate subsequent spectra. In 1999 and
        2000, Lewis and Sommer reported on the approach taken by Nakano
        and Kawata, but on a commercial Perkin Elmer  i-series micro-
        scope. 25,26  In this microscope, the hemisphere with attached sample
        was scanned off-axis, but the sample was illuminated globally and
        only the primary image plane possessed a confocal aperture. Lewis
        and Sommer demonstrated that one-dimensional ATR maps could be
        obtained with improved spatial resolution over a transmission mea-
        surement, but due to diffraction effects associated with the confocal
        aperture, the theoretical improvement in spatial resolution was not
        realized. Further, ATR analysis was capable of measuring a sample 4
        times smaller than that associated with transmission with equal signal
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