or with ξ1 and ξs in Equation (4.18),
and
with φ from Equation (4.22).
We continue with the normalized matrices M:
Based on Equation (4.17), we can represent T(ε)R(ε) with the known matrices D in Equation (4.26) and M in Equation (4.31) as
(4.32)
[T (ε) R (ε)]2πd/pε in Equation (4.14) assumes the form
(4.33)
The evaluation of D2πd/pε, with dε in Equation (4.5) and D in Equation (4.26), provides
(4.34)
K′ in Equation (4.25) leads to
As both the numerator and denominator tend to zero for ε → 0, the application of Hopital’s rule is needed, yielding
The repetition of Hopital’s rule provides
As the denominator of the last equation is identical with limε → 0k′/(2π/p) in Equation (4.35), we obtain
ensuring
(4.37)
The limit of M in Equation (4.31) is calculated in the following steps with φ = arctan
(4.38)
and
With similar calculations as performed for D, we obtain the limit as
(4.39)
and in the same way, also
(4.40)
For the magnitudes the evaluation of the limit value is performed at the square of the magnitudes in Equations (4.29) and (4.30), again leading with similar calculations as for D to
(4.41)
and
(4.42)
Hence, the normalized M is, for ε → 0,
from which, as M is a unitary matrix, we obtain
Inserting Equations (4.29), (4.30), (4.43) and (4.44) into Equation (4.28) provides, for ε → 0,
with