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240   Chapter Eleven

          The reflectivity of a surface coated with one thin film is given by the
        equation
                                 r   r   2r r cos X
                                       2
                                   2
                                  1
                                       2
                                             1 2
                          R                                         (11.3)
                                      2
                                1   r r   2r r cos X
                                        2
                                     1  2     1 2
        where
                                     4 n t cos I
                                         1 1
                                                1
                              X                                     (11.4)

                             sin (I 0   I 1)   tan (I 0   I 1)
                       r                   or                       (11.5)
                        1
                             sin (I   I )      tan (I   I )
                                  0   1             0    1
                             sin (I 1   I 2)   tan (I 1   I 2)
                       r                   or                       (11.6)
                        2
                             sin (I   I )      tan (I   I )
                                  1   2             1    2
        and 	 is the wavelength of light; t is the thickness of the film; n 0 , n 1 ,
        and n 2 are the refractive indices of the media; and I 0 , I 1 , and I 2 are
        the angles of incidence and refraction. Figure 11.2 shows a sketch of
        the film and indicates the physical meanings of the symbols. The sine
        or tangent expressions for r 1 and r 2 are chosen depending on the polari-
        zation of the incident light as in Eq. 11.1; for unpolarized light, which
        is composed equally of both polarizations, R is computed for each polari-
        zation and the two values are averaged. If we assume nonabsorbing
        materials, the transmission T equals (1   R). At normal incidence I 0
        I 1   I 2   0, and r 1 and r 2 reduce to
                                        n   n
                                         0
                                   r          1                     (11.7)
                                   1    n   n
                                         0    1
                                        n 1   n 2
                                   r                                (11.8)
                                   2    n   n
                                         1    2











                                       Figure 11.2 Passage of light ray
                                       through a thin film, indicating
                                       the terms used in Eq. 11.3.
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