Ultrahigh-Speed Optical Transmission Technology (Optical and by Hans-Georg Weber, Masataka Nakazawa

By Hans-Georg Weber, Masataka Nakazawa

This booklet is an in depth description of all of the features of ultrahigh velocity optical transmission expertise. Ultrahigh-speed optical transmission expertise is a key know-how for expanding conversation capability. The units constructed for ultrahigh-speed optical transmission aren't constrained to communique purposes merely. they're key units for high-speed optical sign processing, i.e. tracking, dimension and regulate, and may therefore supply a large technological foundation for cutting edge technological know-how and expertise. a lot of these facets of ultrahigh-speed optical transmission know-how are defined intimately during this book.

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L. A. Jiang, M. E. Grein, and E. P. lppen, "Region of validity for residual phase noise measurements of actively modelocked lasers" submitted to Electron. Lett. 80. H. Shi, D. Cohen, J. Barton, M. Majewski, L. A. Coldren, M. C. Larson, and G. A. Fish, "Relative intensity noise measurements of a widely tunable sampled-grating DBR laser," IEEE Photon. Technol. , 14 (6), 759-761 (2002). 81. P. Scott, C. Langrock, and B. H. Kolner, "High-dynamic-range laser amplitude and phase noise measurement techniques" IEEE.

Haus, L. A. Jiang, and E. E Ippen, "Action on pulse position and momentum using dispersion and phase modulation," Opt. Express, 8 (12), 664-669 (2001). 83. A. Jiang, M. E. Grein, H. A. Haus, E. P. lppen, and H. Yokoyama, "Timing jitter eater for optical pulse trains" Opt. , 28 (2), 78-80, 2003. 84. L. Mollenauer and C. Xu, "Time-lens timing-jitter compensator in ultra-long haul dwdm dispersion managed soliton transmissions;' in CLEO'02 Postdeadline Papers, 2002. 85. Thomas R. Clark Irl N. Duling III, Robert P.

For EDFLs, N is typically on the order of 10000, which 3 This is a good approximationin EDFLswherethe gain-lifetimeis long, but may be less appropriatefor semiconductorlasers wherethe gain stronglycorrelatesneighboringpulses. 40 Leaf A. Jiang, Erich P. Ippen, and Hiroyuki Yokoyama Fig. 11. Temperature-controlled external cavity mode-locked semiconductor laser with 5-nm filter for two different modulation depths. means that to correctly measure the noise, one must run 70000 measurements! If we assume that neighboring pulses are uncorrelated, then all the Lorentzian spectra have the same height and only 7 measurements are needed.

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