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CHARACTERIZATION OF HALF-TONE PRINTERS                 147
             Equation (9.6)] has been shown to be most accurate (Bala, 2003). In the n-
             modified Neugebauer model all the reflectances are raised to the power 1/n as in
             Equation (9.5).
               In order to implement the Neugebauer approach the digital counts are first
             converted into the dot coverage areas using a tone-reproduction curve, as
             described in the previous section. A method to compute the actual areas of the
             primary and secondary colours is then required. For the three-colour example,
             the proportional areas of the eight colour regions can be computed using
             Demichel’s equation (Green, 2002c),
                  A w ¼ð1   cÞð1   mÞð1   cÞ,
                   A c ¼ cð1   mÞð1   yÞ,
                  A m ¼ mð1   cÞð1   yÞ,
                  A y ¼ yð1   cÞð1   mÞ,
                                                                                 ð9:7Þ
                  A b ¼ cmð1   yÞ,
                  A g ¼ cyð1   mÞ,
                   A r ¼ myð1   cÞ,
                  A k ¼ cmy,
             where c, m and y are the proportional dot areas of the three primary colours
             obtained from the tone-reproduction curves. Demichel’s equation has been
             shown (Viggiano, 1990) to work reasonably well for rotated half-tone screen
             configurations where the screens for cyan, magenta and yellow are placed at
             different angles that are carefully selected to avoid moire ´ artifacts.
               It is important to note, however, that Equations (9.7) make certain
             assumptions concerning the amount of overlap between the primary colours.
             If we consider the case where c ¼ 0.4, y ¼ 0.4 and m ¼ 0, then Demichels’s
             equation will predict A ¼ 0.36, A ¼ 0.24, A ¼ 0.24 and A ¼ 0.16. However, it
                                  w         c        y            g
             would be possible for the cyan and magenta dots to be printed without overlap
             (A ¼ 0.20, A ¼ 0.40, A ¼ 0.40 and A ¼ 0.00), with total overlap (A ¼ 0.60,
               w
                                                                             w
                                   y
                         c
                                                g
             A ¼ 0.00, A ¼ 0.00 and A ¼ 0.40) or with any intermediate amount of overlap.
                        y
                                     g
              c
             The primaries normally are printed at different screen angles and the relationship
             between these two angles is one of several factors that could affect the degree of
             overlap. The dot-on-dot half-tone configuration, for example, places the primary
             dots at the same screen angle and phase so that they maximally overlap. In
             practice it has been shown that a weighted combination of the Demichel model
             and the dot-on-dot model can give good performance (Bala, 2003).
             9.4.3  The Kubelka–Munk model

             The Neugebauer models assume that the reflectance (for spectral Neugebauer
             approaches) or tristimulus values (for tristimulus Neugebauer approaches) are
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