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Optical Coatings  245

        where the symbol |z| indicates the modulus of a complex number z, so
        that

                            |z|   |x   iy|    x   y  2
                                                2
        and
                                           x   iy 1   2  x   y  2
                                                       2
                                          1
                                                       1
                           2
                                2
                                                            1
                                    2
                    R   |z|   x   y                          2
                                         x   iy
                                                       2
                                          2     2     x   y 2
                                                       2
        If the computation has been for normal incidence through nonabsorb-
        ing materials, the transmission is given by
                                    T   1   R                      (11.18)
        Otherwise, the transmission is given by
                                                   2
                                    n 0 cos   0  E 0
                               T                                  (11.19a)

                                    n cos      E
                                     p     p   p
        or
                                    n cos     E     2
                                               0
                                     0
                               T           p                      (11.19b)

                                    n cos      E p
                                     p     0
        where Eq. 11.19a is used for light polarized with the electric vector
        perpendicular to [s] and Eq. 11.19b for the electric vector parallel to [p]
        the plane of incidence.
          A discussion of the design of multilayer coatings is beyond the scope
        of this volume; the interested reader should pursue the subject in the
        references listed at the end of this chapter. By suitable combinations of
        thin films of different indices and thicknesses a tremendous number
        of transmission and reflection effects can be created. Among the types
        of interference coatings which are readily available are long- or short-
        pass transmission filters, bandpass filters, narrow bandpass (spike fil-
        ters), achromatic extra-low-reflection coatings as well as the reflection
        coatings described in the next section. An extremely valuable property
        of thin-film coatings is their spectral versatility. Once a combination of
        films has been designed to produce a desired characteristic, the wave-
        length region can be shifted at will by simply increasing or decreasing
        all the film thicknesses in proportion. For example, a spike filter
        designed to transmit a very narrow spectral band at 1   m can be
        shifted to 2  m by doubling the thickness of each film in the coating.
        This, of course, is limited by the absorption characteristics of the sub-
        strate and the film materials.
          The characteristics of a number of typical interference coatings are
        shown in Fig. 11.5. Note that the wavelength scale is plotted in arbitrary
        units, with a central wavelength of 1, since (within quite broad limits)
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