D¼
n^21 n^22
2n^21
n 1 n 2
n 1
ð 3 : 11 Þ
The approximation on the right-hand side reduces this expression forΔto that of
the step-indexfiber. Thus, the same symbol is used in both cases. Forα=∞, inside
the core Eq. (3.10) reduces to the step-index profile n(r) = nl.
3.2.2 Graded-Index Numerical Aperture
Whereas for a step-indexfiber the NA is constant across the core end face, in
graded-indexfibers the NA is a function of position across the core end face. Thus
determining the NA is more complex for graded-indexfibers. Light incident on the
fiber core end face at a position r will be a guided mode only if it is within thelocal
numerical apertureNA(r) at that point. This parameter is defined as [ 6 ]
NA(rÞ¼n^2 ðrÞn^22
(^1) = 2
NAð 0 Þ
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
1 ðÞr=aa
q
for ra
¼0 for r[a
ð 3 : 12 Þ
where theaxial numerical apertureis defined as
NAð 0 Þ¼n^2 ð 0 Þn^22
(^1) = 2
¼ n^21 n^22
1 = 2
n 1
ffiffiffiffiffiffi
2 D
p
ð 3 : 13 Þ
Thus, the numerical aperture of a graded-indexfiber decreases from NA(0) to
zero for values of r ranging from thefiber axis to the core edge. In a graded-index
fiber the number of bound modes Mgis [ 1 ]
Mg¼
a
aþ 2
2 pa
k
2
n^21 D
a
aþ 2
V^2
2
ð 3 : 14 Þ
Typically a parabolic refractive index profile given byα= 2.0 is selected by
fiber manufacturers. In this case, Mg=V^2 /4, which is half the number of modes
supported by a step-indexfiber (for whichα=∞) that has the same V value.
Example 3.8Consider a 50-μm diameter graded-index fiber that has a
parabolic refractive index profile (α= 2). If thefiber has a numerical aperture
NA = 0.22, how many guided modes are there in thefiber at a wavelength of
1310 nm?
3.2 Graded-Index Optical Fibers 65