A bit error rate (BER) analysis for the Non-linear Optical Loop Mirror (NOLM) demultiplexer is presented using a combined optical receiver and NOLM model. The control pulse used in the NOLM model is assumed to be of soliton shape in order to obtain a flat-top switching window to reduce the effect of timing jitter between the control and signal pulses. The NOLM model is incorporated into an optical receiver model for a bit error rate (BER) analysis. It is found that noise due to timing jitter, cross-talk and BER are strongly dependent on the walk-off time between the control and signal pulses in the NOLM demultiplexer. Results show that the power penalty of a NOLM demultiplexer using a soliton control pulse can be minimized with an optimum value of walk-off time. In addition the cross-talk of the Terahertz Optical Asymmetric Demultiplexer (TOAD) has been investigated using a TOAD model. Simulation results show that the cross-talk of a TOAD increases as the asymmetry time is increased. A comparison of the two devices for 100 Gb/s demultiplexing shows that the cross-talk of a TOAD (with an optical amplifier recovery time of 300 ps) is at least 3 dB lower than that of NOLM for maximum demultiplexed output.
[1]
N. Olsson.
Lightwave systems with optical amplifiers
,
1989
.
[2]
Zabih Ghassemlooy,et al.
Modelling of semiconductor laser amplifier for the terahertz optical asymmetric demultiplexer
,
1998
.
[3]
J. P. Sokoloff,et al.
A terahertz optical asymmetric demultiplexer (TOAD)
,
1993,
IEEE Photonics Technology Letters.
[4]
W. Pieper,et al.
SLALOM: semiconductor laser amplifier in a loop mirror
,
1995
.
[5]
Toshio Morioka,et al.
Signal-to-noise ratio analysis of 100 Gb/s demultiplexing using nonlinear optical loop mirror
,
1997
.
[6]
H. Takara,et al.
Effects of control-signal pulse walk-off on BER performance of nonlinear optical loop mirror demultiplexer
,
1993
.
[7]
M. Jinno,et al.
Nonlinear Sagnac interferometer switch and its applications
,
1992
.