described with the help of abbreviated equations for the electric field strength E L and
the laser optical phase φ:
dE L =dt ¼ α 0L À 2πν 0P =Q 0L
ð
ÞÀβ 0n E L
2
Â
Ã
E L À ξ βAN ,
ð6:2Þ
Fig. 6.7 Different types of the MZ modulator (а) and (b) with electrodes connecting to optical
channels OC1 and OC2 in the electro-optical Mach–Zehnder modulator of the microwave range
6.3 Mathematical Model of OEO MZ
295
the laser optical phase φ:
dE L =dt ¼ α 0L À 2πν 0P =Q 0L
ð
ÞÀβ 0n E L
2
Â
Ã
E L À ξ βAN ,
ð6:2Þ
Fig. 6.7 Different types of the MZ modulator (а) and (b) with electrodes connecting to optical
channels OC1 and OC2 in the electro-optical Mach–Zehnder modulator of the microwave range
6.3 Mathematical Model of OEO MZ
295