The design of opticle thin films requires knowledge of the reflecting
coefficient r(omega), (omega, a complex variable). However, as \r(omeg
a)\ is measurable only, we have to construct a phase Phi(omega), so th
at r(omega) = \r(omega)\e(i Phi(omega)) is a holomorphic complex funct
ion. This problem is solved by using a generalized Schwarz formula and
the boundary values are computed.