modes that propagate along the z axis, form a standing wave along the x axis in
region 1, and decay exponentially in region 2. The same result can be obtained by
solving the wave equation over the regions and matching boundary conditions at
the interfaces. The guided mode is said to be cutoff when u
1
u
c
, where k
2
is real
and b n
2
k
0
. An unguided wave below cutoff that nevertheless meets the
transverse resonance conditions is sometimes known as a ‘‘leaky wave.’’
2.3.3 Optical Fiber: A Cylindrical Waveguide
The ray optics analysis for a cylindrical waveguide such as an optical fiber is
complicated by the existence of skew rays in three dimensions, which propagate
helically and do not cross the fiber axis. Here, we outline the solution of the field