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98    Cha pte r  F o u r


                          Calculated IR Transmission for Amtir 4
                              Absorption
          Wavelength   Refractive   Coefficient   Thickness
                                 −1
          (µm)       IR Index  (cm )    (cm)      Reflectivity  Transmission
                                   Fiber Results
           1.00      2.7788   0.04      2.6       0.221588  0.568757
           1.50      2.6995   0.005     2.6       0.211036  0.642296
           2.00      2.6778   0.003     2.6       0.208115  0.649923
           2.5       2.6686   0.003     2.6       0.206873  0.651618
           3.00      2.6637   0.002     2.6       0.20621   0.654372
           4.00      2.6588   0.002     2.6       0.205547  0.655281
           5.00      2.6561   0.002     2.6       0.205181  0.655783
           6.00      2.6541   0.001     2.6       0.20491   0.658012
           7.00      2.6524   0.001     2.6       0.204679  0.658329
           8.00      2.6508   0.001     2.6       0.204462  0.658628
           9.00      2.6491   0.009     2.6       0.204231  0.644245
          10.00      2.6472   0.012     2.6       0.203973  0.639178
          11.00      2.6452   0.014     2.6       0.203702  0.635961
          12.00      2.643    0.024     2.6       0.203403  0.618777
          13.00      2.6407   0.35      2.6       0.20309   0.257349
          14.00      2.638    0.47      2.6       0.202723  0.187959

        TABLE 4.2  AMI Program to Calculate Transmission of Amtir 4 as a Function of
        Thickness and Wavelength


              incorporating absorption coefficient results calculated from the plate
              scan. Table 4.2 illustrates this procedure when applied to Amtir 4.
                 Specifications for wavelengths less than 2 µm (NIR) require the use
              of a different kind of an instrument. In this case, the AMI Beckman
              UV 5240 spectrophotometer covers the wavelength range of 0.5 to
              2.5 µm. AMI uses a reflection attachment specifically designed for the
              instrument to evaluate antireflection coating results. The attachment
              mounts inside the sample area that may be closed when it is neces-
              sary to keep light out of the instrument. In double-beam operation,
              the instrument is an electronic null instrument not designed for high-
              index solid materials. Care must be exercised in taking measure-
              ments, and the results must be carefully evaluated. The fundamental
              absorption edge, where the glasses begin to transmit, cannot be mea-
              sured using either of the FTIR instruments. The Beckman instrument
              must be used. As an example, a plot of the transmission edge for an
              8-in-diameter Amtir 4 glass plate is shown in Fig. 4.7. Notice the plate
              is 2.6 cm thick.
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