Abstract
Dark solitons1 are characterized by an intensity dip on a continuous background, which propagates unaltered. Although a true continuous background wave may be impractical, it has been shown that dark pulses on a background pulse of finite width can propagate adiabatically as solitons.2 Dark solitons have been observed in optical fibers by a few different experimental techniques3; however, the generation of the dark soliton trains from the interference and nonlinear copropagation of two delayed visible pulses in an optical fiber is numerically investigated.
© 1991 Optical Society of America
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