All-optical clock extraction using two-contact devices

A comprehensive summary of the operation of two-contact semiconductor self-pulsating laser diode (SP—LD) in both return-to-zero (RZ) and non-return-to-zero (NRZ) optical transmission systems is presented. Results demonstrate that this type of device has great potential as the basis for all-optical clock recovery circuits at multi-Gbits rates for switching applications. Results describe the basic device behaviour showing how zinc doping the shorter (absorber) region of the device enables repeatable and controlled GHz pulsations, within the range ∼ 0.6 to > 5.5 GHz and tunability (via the DC gain current) over many GHz, to be achieved. Experimental results show that the SP-LD can be locked with μW of incident power to produce a locked oscillator with a linewidth of < 10 Hz at 5 GHz and with 20 dB power gain across the device. New results, addressing the pattern dependence, demonstrate that long breaks (up to ∼ 30 ‘zeros’) in the clock can be accommodated without significant degradation of the locked clock purity; the length of break being dependent on the initial state of locking. Other new results show that the lock-up time for such circuits is of the order of 100 clock cycles. System performance is investigated using these devices within a 20 Gbit/s (4 × 5 Gbit/s) optical-time-division-multiplexed demonstrator; the results showing no significant degradation of the bit-error-ratio performance. Other system results at 3.2 Gbit/s show that this technique can be applied to NRZ systems when also utilising a nonlinear effect within a similar device biased below threshold, and identifying the differences from RZ operation. These results show that such an approach could provide major benefits in developing the next generation of telecommunications networks.

[1]  G. Olsen,et al.  Self-oscillations and dynamic behavior of aged InGaAsP laser diodes , 1981 .

[2]  M. Jinno,et al.  All-optical timing extraction using an optical tank circuit , 1990, IEEE Photonics Technology Letters.

[3]  All-optical synchronisation with frequency division using selfpulsating laser diode , 1992 .

[4]  Charles Howard Henry,et al.  Theory of defect‐induced pulsations in semiconductor injection lasers , 1980 .

[5]  D. M. Spirit,et al.  20 Gbit/s, 205 km optical time division multiplexed transmission system , 1991 .

[6]  Roy Lang,et al.  Conditions for self-sustained pulsation and bistability in semiconductor lasers , 1985 .

[7]  M. Honsberg Controlled generation of optical pulse trains by double-contacted GaAs laser diodes , 1984 .

[8]  W. Pieper,et al.  Decision gate for all-optical data retiming using a semiconductor laser amplifier in a loop mirror configuration , 1993 .

[9]  R. Olshansky,et al.  Measurement of radiative and nonradiative recombination rates in InGaAsP and AlGaAs light sources , 1984 .

[10]  H. Serizawa,et al.  Effect of device parameters on bistable semiconductor laser , 1986 .

[11]  W. Joyce,et al.  A possible model for sustained oscillations (pulsations) in (Al,Ga)As double-heterostructure lasers , 1979 .

[12]  E. Avrutin,et al.  Analysis of spontaneous emission and noise in self-pulsing laser diodes , 1993 .

[13]  M. Saruwatari,et al.  10 GHz timing extraction from randomly modulated optical pulses using phase-locked loop with travelling-wave laser-diode optical amplifier using optical gain modulation , 1992 .

[14]  T. Kamiya,et al.  Observation of Chaos in an Inhomogeneously Pumped Self-Pulsating Semiconductor Laser , 1989 .

[15]  All-optical synchronization and multiplication of the frequency of mode-locked signals , 1992, IEEE Photonics Technology Letters.

[16]  Clock extraction using saturable absorption in a semiconductor nonlinear optical amplifier , 1991, IEEE Photonics Technology Letters.

[17]  J. Gamelin,et al.  Pulsation stabilization and enhancement in self-pulsating laser diodes , 1992, IEEE Photonics Technology Letters.