1997
DOI: 10.1109/68.554532
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Experimental demonstration of soliton transmission over 28 Mm using mostly normal dispersion fiber

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1997
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Cited by 65 publications
(15 citation statements)
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“…Since the amplifier gain evolves on a time-scale of milliseconds, while evolves on a time-scale of picoseconds, we must use a multiple time/length-scale approach in which we average over the rapid variations of to determine the evolution of the gain and then fix the gain to determine the evolution of [22]. If we consider the evolution of the gain coefficient of the th amplifier in the loop, then its gain coefficient may be written (4) where is the normalized time; in contrast to used in (1), is unretarded. The distance is internal to the amplifier so that and is normalized with respect to .…”
Section: Model and System Parametersmentioning
confidence: 99%
“…Since the amplifier gain evolves on a time-scale of milliseconds, while evolves on a time-scale of picoseconds, we must use a multiple time/length-scale approach in which we average over the rapid variations of to determine the evolution of the gain and then fix the gain to determine the evolution of [22]. If we consider the evolution of the gain coefficient of the th amplifier in the loop, then its gain coefficient may be written (4) where is the normalized time; in contrast to used in (1), is unretarded. The distance is internal to the amplifier so that and is normalized with respect to .…”
Section: Model and System Parametersmentioning
confidence: 99%
“…21 Since transmission systems are generally in normal dispersion regions where group velocity is smaller than c, group delay distortions are caused by the lagging group delay. [22][23][24] So far, various dispersion compensation schemes have been proposed to eliminate group delay distortion in optical fiber transmission. digital compressors, and in-line amplifiers.…”
Section: Introductionmentioning
confidence: 99%
“…We note that source noise by itself can limit the transmission distance [8], but it is not a major factor in our experiments [7].…”
Section: Introductionmentioning
confidence: 99%
“…However, in real systems the initial puls differs from the final soliton shape. The pulses pass through a complex transient regime before transforming into solitons [7], and propagation in the transient regime can be as long as 10 000 km. Our analysis shows that when the initial pulses have slowly dropping tails, the interpulse interaction in the transient regime can be significantly stronger than the interpulse interaction in the soliton regime.…”
Section: Introductionmentioning
confidence: 99%
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