argument. The normalized transverse propagation and decay constants are
defined, respectively, as
u ¼ b
t1
a ¼ a(n
2
1
k
2
0
b
2
)
1=2
and w ¼ b
t2
jj
a ¼ a(b
2
n
2
2
k
2
0
)
1=2
: (2:10a)
Then the complete solution can be written as
E
z
¼ AJ
q
(ur=a) sin (qf) exp (jbz) for r a, and (2:10b)
E
z
¼ CK
q
(wr=a) sin (qf) exp (jbz) for r a: (2:10c)
Note that the f and z dependences are identical in the core and cladding, as
expected by intuition, with the solutions differing only in the radial dependence.
The form of the solution for E
r
, E
f
, H
r
, H
z
, and H
f
can be derived from the
solution for E
z
using the Maxwell equations. The solutions are characterized by
q, the mode order, or azimuthal mode number, which takes on integer values
q ¼ 0, 1, 2, and so on. The eigenvalues are the ...