Abstract
The combination of the chirp of directly modulated semiconductor lasers and the chromatic dispersion of conventional single-mode fiber results in intersymbol interference which can cause significant performance degradations (e.g., see Refs. 1-3). Figure 1 shows a 1.55-μm fiber optic communication system using intensity modulation and direct detection. The laser is directly modulated at 8 Gbit/s. The current pulses (either NRZ or RZ with a 75% duty cycle) are square pulses distorted by laser parasitics and intentional filtering; we assume an equivalent overall response identical to that of an RC circuit with a 4-GHz bandwidth. The laser output is transmitted over an L-km length of single-mode fiber, which has a transfer function Hf(ω) = exp[j(Lλ2Dω2)/(4πc)], where D, the fiber dispersion parameter, is 17 ps/nm/km. The fiber output is passed through the photodetector and receiving filter (third-order Butterworth with a bandwidth of 6.24 GHz). In the equalized system, the fiber output is first operated by the equalizing Heq(ω) before passing on to the photodetector. The control loop (Fig. 1) represents the means for adapting the frequency position of Heq(ω).
© 1990 Optical Society of America
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