Optical data synchronization using tunable transmitters and nonzero dispersion links

A new digital feedback loop for synchronizing optical data with a clock at an arbitrary point in a fiber-optic link has been experimentally demonstrated and its physical limitations have been analyzed. The feedback loop consists of a tunable transmitter, a nonzero dispersion link, and standard microwave and digital electronics. The feedback loop was able to suppress thermal fluctuations with an accuracy better than 1 ps using either a temperature tuned DFB laser diode or a current tuned DBR laser diode. No bit-error rate penalty was measured during closed loop operation compared to back-to-back transmission. The physical limitations of the loop stem from noise in the receiver and the actuator increment. Thermally induced phase fluctuations in the fiber at frequencies above the loop bandwidth were found negligible. The maximum experimental delay time for stable operation was 0.86 s, indicating the possibility of closed loop operation for very long fiber links. The feasibility of packet synchronization is discussed. Moreover, a new scheme is proposed to circumvent wavelength reset when the system approaches the operating boundaries. >

[1]  S. Kawanishi,et al.  Ultra-high-speed PLL-type clock recovery circuit based on all-optical gain modulation in traveling-wave laser diode amplifier , 1993 .

[2]  Berthold Wedding Wedding Dispersion-supported transmission at 1550 nm on long spans of conventional single-mode fiber , 1994 .

[3]  Mark J. W. Rodwell,et al.  Subpicosecond laser timing stabilization , 1988 .

[4]  All-optical frame synchronisation recovery , 1994 .

[5]  Toshio Morioka,et al.  100 Gbit/s, 200 km optical transmission experiment using extremely low jitter PLL timing extraction and all-optical demultiplexing based on polarisation insensitive four-wave mixing , 1994 .

[6]  G. Agrawal Fiber‐Optic Communication Systems , 2021 .

[7]  T. Tanbun-Ek,et al.  32 Gb/s optical soliton data transmission over 90 km , 1992, IEEE Photonics Technology Letters.

[8]  Richard A. Thompson Architectures with improved signal-to-noise ratio in photonic systems with fiber-loop delay lines , 1988, IEEE J. Sel. Areas Commun..

[9]  M. Saruwatari,et al.  Multi-WDM-channel, Gbit/s pulse generation from a single laser source utilizing LD-pumped supercontinuum in optical fibers , 1994, IEEE Photonics Technology Letters.

[10]  H. Ishii,et al.  Tuning-current splitting network for three-section DBR lasers , 1994 .

[11]  Paul R. Prucnal,et al.  Optically processed self-routing, synchronization, and contention resolution for 1-D and 2-D photonic switching architectures , 1993 .

[12]  A. Dandridge,et al.  Measurements of fundamental thermal induced phase fluctuations in the fiber of a Sagnac interferometer , 1995, IEEE Photonics Technology Letters.

[13]  H.J. Wickes,et al.  All-optical clock recovery from 5 Gb/s RZ data using a self-pulsating 1.56 mu m laser diode , 1991, IEEE Photonics Technology Letters.

[14]  P. Blixt,et al.  An optical technique for bit and packet synchronization , 1995, IEEE Photonics Technology Letters.

[15]  John E. Bowers,et al.  Comparison of timing jitter in external and monolithic cavity mode‐locked semiconductor lasers , 1991 .

[16]  Zygmunt J. Haas,et al.  The 'staggering switch': an electronically controlled optical packet switch , 1993 .

[17]  Gene F. Franklin,et al.  Digital control of dynamic systems , 1980 .

[18]  Edward I. Ackerman,et al.  Hybrid guided-wave optical time delay switch , 1994 .

[19]  Masahiko Jinno,et al.  Optical tank circuits used for all-optical timing recovery , 1992 .

[20]  K. Smith,et al.  All-optical clock recovery using a mode-locked laser , 1992 .

[21]  K. Wanser,et al.  Fundamental phase noise limit in optical fibres due to temperature fluctuations , 1992 .