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  • Key words. nonlinear dispersive fibers, nonsoliton pulses, onset of oscillations, hyperbolic shocks  (1)
  • numerical simulation  (1)
  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of nonlinear science 8 (1998), S. 43-62 
    ISSN: 1432-1467
    Keywords: Key words. nonlinear dispersive fibers, nonsoliton pulses, onset of oscillations, hyperbolic shocks
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Summary. We study the modulation equations for the amplitude and phase of smoothed rectangular pulse initial data for the defocusing nonlinear Schrodinger (NLS) equation in the semiclassical limit, and show that these equations exhibit shock formation. In this way we identify and explain one source for the onset of pulse oscillations in nonlinear fibers whose transmission is modeled by the semiclassical NLS equation. The onset of pulse ripples predicted here develops on the leading and trailing slopes of a smooth pulse, as a consequence of shock formation in the modulation equations. This mechanism for the onset of pulse ripples is distinct, both in the location and timescale, from the scenario pursued by Kodama and Wabnitz [11]: A piecewise linear pulse evolves for distances O(1) down the fiber, beyond which oscillations develop associated with the vanishing of the upper step of the pulse [10]. Here we show that the scenario in [11] is correct, but specific to pure rectangular pulses ; any smoothing of this data fails to obey their scenario, but rather is described by the results presented here. That is, the semiclassical limit of the NLS equation is highly unstable with respect to smooth regularizations of rectangular data. In our analysis, the onset of oscillations is associated with the location of the maximum gradient of the pulse slopes, and onset occurs on the pulse slopes, at short distances down the fiber proportional to the inverse of this maximum gradient. Explicit upper and lower bounds on the initial shock location are derived. We thereby deduce the onset for this source of pulse degradation scales linearly with the pulse width, and scales with the reciprocal square root of the fiber nonlinear coefficient, the pulse power, and the fiber dispersion coefficient.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of nonlinear science 3 (1993), S. 393-426 
    ISSN: 1432-1467
    Keywords: nearly integrable PDE ; nonlinear modes ; modulation equations ; numerical simulation
    Source: Springer Online Journal Archives 1860-2000
    Topics: Mathematics , Physics
    Notes: Summary The purpose of this paper is the derivation of reduced, finite-dimensional dynamical systems that govern the near-integrable modulations ofN-phase, spatially periodic, integrable wavetrains. The small parameter in this perturbation theory is the size of the nonintegrable perturbation in the equation, rather than the amplitude of the solution, which is arbitrary. Therefore, these reduced equations locally approximate strongly nonlinear behavior of the nearly integrable PDE. The derivation we present relies heavily on the integrability of the underlying PDE and applies, in general, to anyN-phase periodic wavetrain. For specific applications, however, a numerical pretest is applied to fix the truncation orderN. We present one example of the reduction philosophy with the damped, driven sine-Gordon system and summarize our present progress toward application of the modulation equations to this numerical study.
    Type of Medium: Electronic Resource
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