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c
n .
ν =
(6)
Implementing this equation to the phase and group velocities, the formulae for
the phase and group refractive indices n ph and n gr read
c
n ph ,
ν ph =
(7)
c
n gr .
ν gr =
(8)
λ
Differentiating Eq. 7 with respect to
yields
d
ν ph
d
c
n ph
dn ph
d
=−
.
(9)
λ
λ
Substituting Eqs. 9 , 8 , and 7 into Eq. 5 yields
c
n gr =
c
n gr + λ
c
n ph
dn ph
d
,
(10)
λ
or
1
.
1
n gr =
1
n ph
1
n ph
dn ph
d
+ λ
(11)
λ
=
+ ε) 1
Using the approximation
(
1
1
ε
, valid for small quantities of
ε
,Eq. 11
is inverted to
n ph 1
1
n ph
dn ph
d
n gr =
λ
.
(12)
λ
Thus the group refractive index follows
dn ph
d
n gr =
n ph λ
,
(13)
λ
Equation 13 is the modified Rayleigh equation (Hofmann-Wellenhof et al. 1993 ).
A slightly different form is obtained by differentiating the relation c
= λ
f with
respect to
λ
and f , that is
d
λ
λ
df
f ,
=−
(14)
and by substituting the results into Eq. 13 , the group refractive index yields
dn ph
df .
n gr =
n ph +
f
(15)
 
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