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Soliton propagation in long fibers with periodically compensated loss
340
Citations
13
References
1986
Year
Soliton PropagationPhotonicsEngineeringOptical AmplificationPhysicsOptical Transmission SystemOptical PropertiesOptical TransmissionNonlinear Wave PropagationOptical SolitonClassical OpticsSoliton PeriodsFiber OpticsLow Soliton PowersOptical SystemsOptical CommunicationFiber OpticFiber-optic Communication
With computer simulation, we study soliton propagation in an all-optical, long-distance communications system where fiber loss is periodically compensated by Raman gain. We find that distortion of the transmitted pulses from true solitons shows a peak near <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">z_{0} = L/8</tex> where <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">L</tex> and z <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0</inf> are the amplification and soliton periods, respectively. We also describe optimal system design based on the exceptional pulse stability and low soliton powers obtained in the region <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">z_{0} \gg L/8</tex> . Typical amplification periods are in the range 30-50 km, pump powers are less than 100 mW, and for bit rates in the 10 GHz range, time average signal powers are at most a few milliwatts. The single-channel rate-length product for error rate less than 10 <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-9</sup> is <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">\sim29 000</tex> GHz Km. Finally, we show that in the gain-compensated system with wavelength multiplexing, soliton-soliton collisions produce random modulation of individual pulse velocities. Nevertheless, multiplexing can yield rate-length products greater than 300 000 GHz km.
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