1991
DOI: 10.1109/3.97280
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Generation of fundamental soliton trains for high-bit-rate optical fiber communication lines

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Cited by 204 publications
(55 citation statements)
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“…2, but now we investigate different lengths of fiber and allow for nonuniform changes of and along the fiber, that is, different profiles of and [4]. Our simulations indicate that the shortest fiber length over which the maximum compression can be achieved requires constant effective gain along the fiber [19], [20]. In its dimensionless form, this condition can be written as (2) where is the initial soliton width and is the position along the optimized fiber.…”
Section: Minimized Fiber Length For Adiabatic Compressionmentioning
confidence: 98%
“…2, but now we investigate different lengths of fiber and allow for nonuniform changes of and along the fiber, that is, different profiles of and [4]. Our simulations indicate that the shortest fiber length over which the maximum compression can be achieved requires constant effective gain along the fiber [19], [20]. In its dimensionless form, this condition can be written as (2) where is the initial soliton width and is the position along the optimized fiber.…”
Section: Minimized Fiber Length For Adiabatic Compressionmentioning
confidence: 98%
“…From the point of view of telecom applications, XPolM-MI can be an essential source of nonlinear impairments for WDM systems with polarization interleaving or polarization multiplexing [42][43][44][45]. Also on a more fundamental level, MI is a generic nonlinear process that occurs in many areas, and it is at the origin of very important fundamental phenomena, such as optical soliton generation [46,47], supercontinuum generation [48], and rogue wave formation [29,30,[49][50][51].…”
Section: Theoretical Analysis Of Polarization Modulation Instabilitymentioning
confidence: 99%
“…Some techniques, such as the nonlinear intensity discrimination technique [2,3] can reduce the pedestals, but typically energy is wasted. Adiabatic soliton compression typically utilizes a dispersion map with monotonically decreasing dispersion along the propagation direction, z, and is formally equivalent to distributed amplification [4,5]. If the dispersion varies slowly enough, the soliton self-adjusts to maintain the balance between dispersion and nonlinearity (by reducing its pulse width; hence the term adiabatic compression) [6].…”
Section: Introductionmentioning
confidence: 99%