
548 Handbook of Biomedical Optics
interference of two planar coherent waves each described by a
wave vector of size k at angle ± to the optic axis.
According to the linearity of the Maxwell equations, which
implies that the sum of two amplitude distributions consti-
tutes also a solution of the Maxwell equations (alternatively the
d’Alembert equation), plane light waves can simply be added
(Figure 26.4). Hence the y-component of the electric eld is
written as
E E e E e
i k x z i k x
= +
−
− − ⋅ + ⋅ −
+
− ⋅ +
1 1
1
[ ( sin( ) cos( ) ) ] [ (sin( ) cos(α α φ α α)) ) ]⋅ −z φ
2
(26.7)
Here E
−1
and E
−2
are amplitudes of incident plane light waves,