Page 263 - Modern Optical Engineering The Design of Optical Systems
P. 263

Optical Coatings  243





           4%
          REFLECTANCE  3%       BROADBAND MULTI-LAYER



           2%

           1%           QUARTER-WAVE MgF2
                         V-COATING


                 400      500     600     700     800
                            WAVELENGTH (nm)
        Figure 11.4b The reflectivity of three typical coatings: a single
        quarter-wave layer of magnesium fluoride; a two (or more) layer
        “V-coating”; and  a three (or more) layer broadband ultra-low
        reflectivity coating.



        Thin-film computations
        The following equations can be used to calculate the reflection and trans-
        mission of an interference coating of any number of layers. The equations
        can be used at oblique angles and will accommodate absorbing materi-
        als. They do require a knowledge of complex arithmetic; if not already
        familiar with the subject, the interested reader may wish to consult a
        basic text on complex arithmetic. These equations are the basis of most
        of the computer programs used in the design and evaluation of thin
        films. The formulas given here are taken from Peter Berning, in G. Hass
        (ed.), Physics of Thin Films, vol. 1, Academic, 1963.
          The reflection and transmission characteristics of a “stack” of several
        thin films can be expressed in explicit equations; however, their com-
        plexity increases rapidly with the number of films, and the following
        recursion expressions are usually preferable. The physical thickness
        of each film is represented by t j and the index by n j   N j   iK j (n is the
        complex index,  N is the ordinary index of refraction, and  K is the
        absorption coefficient, which is zero for nonabsorbing materials).
        The  angle of incidence within the  jth film is    j ; and the “effective”
        refractive index is u j   n j cos   j or u j   n j /cos   j (for light polarized with
        the electric vector perpendicular to [s], or parallel to [p], the plane of
        incidence, respectively). Thus, for oblique incidence the calculations
        are carried out for both polarizations and the results are averaged
        (assuming the incident light to be unpolarized and to consist of equal
        parts of each polarization).
   258   259   260   261   262   263   264   265   266   267   268